Dielectric Phenomena In High Voltage Engineering (1920) (logo) Dielectric_Phenomena_In_High_Voltage_Engineering_(1920) (link) Distributed by PeseTrier W See other formats Full text of "Dielectric Phenomena In High Voltage Engineering" COPYKIGHT, 1915, 1920, BY THE BOOK COMPANY, INC. PREFACE TO SECOND EDITION This "scanned" edition the text has been very carefully reviewed and typographical and other errors corrected. It has not been found necessary to make any fundamental' changes. During the last five years important investigations on transient and lightning voltages, high voltage d. c. etc., have been made. Data on these and other recent investigations have been added to the text and the appendix. F. W. PEEK, JB. PlTTSFIELD, MASS. July, 1920. PREFACE TO FIRST EDITION It is the object of the author to give in this book the properties of gaseous, liquid and solid insulations, and methods of utilizing these properties to the best advantage in the problems of high- voltage engineering. Such problems require a knowledge, not only of the laws and mechanism of breakdown of dielectrics as determined by experiment, but also a simple working knowledge of the dielectric circuit. Methods that have proved useful in designing apparatus, transmission lines, insulators, bushings, etc., are discussed and illustrated by practical application. In addition, such subjects as the manner of making extensive engineering investigations and of reducing data, the measurement of high voltages, the effects of impulse and high-frequency voltages, methods of draw- ing dielectric fields, outline of modern theory, various dielectric phenomena, etc., are considered. In all cases where laws and discussions of dielectric phenomena are given, it fc&s been thought best to accompany these with experimental data. Much original work is given, as well -as reference to other in- vestigations. The author's extensive research was made possible by facilities afforded by the Consulting Engineering Department of the General Electric Company, for which acknowledgment is made. _ JCha^Es are due Mr. H. K. Humphrey, and others, who _Jbrrei"gfeatly assisted in the experiments and calculations. F. W. P., JR. , SCHENECTADY, N. Y., April, 1915. CONTENTS P\E PREFACE ....... . . v DIELECTRIC UNITS . X i TABLE OF SYMBOLS , . . xni CHAPTER I INTRODUCTION . i General discussion of energy transfer Experimental plots of di- electric and magnetic fields Analogy between magnetic and dielectric fields Analogy with Hooke s Law. CHAPTER II THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT. 8 (Mathematical Consideration) General treatment of the dielectric field and dielectric circuit with discussion of principles used Parallel planes Field between; . per- mittance, etc Concentric cylinders Permittance or capacity; flux density and gradient Parallel wires Principles used in super- position of fields; determination of resultant fields, equation of equipotential surfaces, lines of force and flux density; permittance; gradient and equigradient surfaces Concentric spheres Spheres Two small equal spheres, field of, and permittance, two large equal spheres, gradient, permittance Conditions for spark-over and local breakdown or corona Collected formulae for common electrodes Combinations of dielectrics of different permittivities Dielectric flux refraction Dielectric m series Dielectric in multiple Flux control Imperfect electric elastivity or absorption in dielectrics; dielectric hysteresis. CHAPTER III VISUAL CORONA . . ... 38 General Summary and Discussion Appearance Chemical action A. C. and D. C. spacing and size of conductor Laws of visual corona formation Theory of corona Electron theory Air films at small spacings Air density Measuring yoltage by corona Conductor material, cables, oil and water on the conductors, humidity. lonization Wave shape, current in wire. Experimental Study and Method of Reducing Experimental Data Tests showing the effects of size and spacing of conductors Air density Temperatu re Barometric pressure Strength of air films Effect of frequency Conductor material, oil, water, dirt, humidity lonization Current in wire Stranded conductors Split conductors. Photographic and Stroloscopic Study Positive and negative corona Corona at different voltages Thickness of corona Oscillograms of corona current, etc vii viii CONTENTS CHAPTER IV P\GK SPARK-OVER .... . . . 79 Definition Condition for spark-over or corona Spark-over be- tween parallel wires, wet and dry Measurements of and method of calculating Wires in a cylinder Needle gap Sphere gap Effect of barometric pressure, temperature, humidity, moisture and rain on spark-over; measurement of voltage by spheres ; calculation of curves; precautions in testing Rupturing energy and dielectric spark lag Law of spark-over, effect of high frequency, oscillatory, and impulse voltages on spark-over, and method of measuring such voltages Insulators and bushings Spark-over of; effect of alti- tude, etc CHAPTER V CORONA LOSS 117 Method of making a large engineering investigation Method of reducing data The quadratic law Loss on very small conductors Effect of frequency, size of conductor and spacing; conductor material and surfaces; air density and humidity The disruptive critical voltage Loss near the disruptive critical voltage; the probability law Loss during storm Loss at very high frequency. CHAPTER VI CORONA AND SPARK-OVER IN OIL AND LIQUID INSULATIONS 153 Liquids used for insulating Physical characteristics of transformer oil Spark-over with different electrodes; effect of moisture; tem- perature Corona in oil Law of spark-over and corona in oil Spark-over of wires, plates and cylinders Resistivity of oil Dis- ruptive energy- Oil films Transient voltages Barriers Com- .parison of high frequency 60 and impulse arc over. CHAPTER VII SOLID INSULATION. 166 Solids used for insulation Dielectric loss Insulation resistance and dielectric strength' Rupturing gradient Methods of testing Law of strength vs. thickness Solid vs. laminated insulations Effect of area of electrodes Impulse voltages and high frequency Cumulative effect of over-voltages of steep wave front Law of strength vs. time , of application Permittivity of insulating materials Energy loss in insulations at high and low frequency Operating temperatures of insulation Surface leakage Solid insulating barriers in oil Impregnation Mechanical Direct current Complete data on permittivity, dielectric strength with time, thickness, etc. CHAPTER VIII THE ELECTRON THEORY . 192 Review of and example of practical application. CONTENTS ix * CHAPTER IX PAGE PRACTICAL CORONA CALCULATION FOR TRANSMISSION LINES . 199 Corona and summary of various factors affecting it Practical corona formulse and their application with problems to illustrate Safe and economical voltages Methods of increasing size of con- ductors Conductors not symmetrically spaced Voltage change along line Agreement of calculated losses and measured losses on commercial transmission lines The corona limit of high-voltage transmission, with working tables and curves. CHAPTER X PRACTICAL CONSIDERATIONS IN THE DESIGN OP APPARATUS WHERE SOLID, LIQUID AND GASEOUS INSULATIONS ENTER IN COMBINATION . 213 Breakdown caused by addition of stronger insulation Corona on generator coils Corona in entrance bushings Graded cable Transformer bushing, oil-filled bushings, condenser type bushing Dielectric field control by metal guard rings, shields, etc. High frequency Dielectric fields Methods of plotting, lines of force, equipotential surfaces, equigradient surfaces Dielectric fields in three dimensions, experimental determination of dielectric fields Effect of ground on the dielectric field between wires Three- phase dielectric fields with flat and triangular spacing of con- ductors Occluded air in insulations Examples of calculations of spark-over between wet wires, ,of sphere curves, of breakdown of insulation for transient voltages, of strength of porcelain, of energy loss in insulation, etc. CHAPTER XI COMPLETE DATA APPENDIX 238 Measured data on corona loss INDEX 257 DIELECTRIC UNITS Electromotive force, volts e volts Gradient g = ~ volts /cm. C Permittance or capacitance or ^ _ kKA = g g 4 ^ io~ 14 farads capacity x x Permittivity or specific capacity relative k (k = 1 for air) 10 9 absolute (air) K = -^-^ 8 84 X 10~ 14 farad cm. cube Elastance 8 = ^ Elastivity angle, function. 6 angle. or elastivity. S sum. SS sum of two sums. n co resistance, mm. millimeter, cm. centimeter. = approximately equal to Note that voltages in measured data are often given to neutral; in such cases the single phase line to line voltages are twice (2), and the three phase (symmetrical) -y/3 times, these values. TABLE OF SYMBOLS xv Permittances or capacities are also frequently given to neutral because it is a great convenience in making calculations. The subscript max. is often used to distinguish between the maximum and root mean square or effective This is done because insulation breakdown generally depends upon the maximum point of the wave. Such voltages may be reduced to effective sine wave by dividing by \/2 Sometimes when the maximum gradient is referred to it means the gradient at the point in the field where the stress is a maximum. These references are made clear in the text for each individual case. Tests were made on single-phase lines unless otherwise noted. Views or theories advanced by the author are always accompanied by sufficient experimental data so that the reader may form conclusions independently. DIELECTRIC PHENOMENA CHAPTER I INTRODUCTION It is our work as engineers to devise means of transmitting energy electrically, from one point to another point, and of con- trolling, distributing, and utilizing this energy as useful work. Conductors and -insulating materials are necessary. Trans- mission problems are principally problems of high voltage and therefore of dielectrics. In order that energy may flow along a conductor, energy must be stored in the space surrounding the conductor. This energy is stored in two forms, electromagnetic and electrostatic. The electromagnetic energy is evinced by the action of the resulting stresses, for instance, the repulsion be- tween two parallel wires carrying current, the attraction of a suspended piece of iron when brought near the wires, or better yet, if the wires are brought up through a -plane of insulating material, and this plane is dusted with iron filings, and gently tapped, the filings will tend to form in eccentric circles about the conductors. These circles picture the magnetic lines of force or magnetic field in both magnitude and direction. This field only exists when current is flowing in the conductors. If now potential is applied between the conductors, but with the far ends open circuited, energy is stored electrostatically. The resulting forces in the dielectric are evinced by an attraction between the conductors; a suspended piece of dielectric in the neighborhood is attracted. If % the conductors are brought through an insulating plane as before, and this is dusted with a powdered dielectric, as mica dust, the dust will tend to form in arcs of circles beginning on one conductor and ending on the other conductor. See Fig. l(a) and (6). The dielectric field is thus made as tangible as the magnetic field. Fig l(c) is an experimental plot of the magnetic and dielectric fields. Fig. l(d) is the mathematical plot. Fig. 1 (c) represents the magnetic and 1 2 DIELECTRIC PHENOMENA dielectric fields in the space surrounding two conductors which are carrying energy. The power is a function of the product of these two fields and the angle between them. In comparing Figs. l(c) and (d) only the general direction and relative density of the fields at different points can be considered. The actual number of lines in Fig. l(c) has no definite meaning. The dielectric lines of force in Fig. 1 (d) are drawn so that one twenty- fourth of the total flux is included between any two adjacent lines. Due to the dielectric fields, points in space surrounding the conductors have definite potentials. If points of a given poten- tial are connected together, a cylindrical surface is formed about the conductor; this surface is called an equipotential surface. Thus, in Fig. l(cf), the circles represent equipotential surfaces. As a matter of fact, the intersection of an equipotential surface by a plane at right angles to a conductor coincides with a magnetic line of force. The circles in Fig. l(cT), then, are the plot of the equipotential surfaces and also of the magnetic lines of force. The equipotential surfaces are drawn so that one-twentieth of the voltage is between any two surfaces. For example: If 10,000 volts are placed between the two conductors, one con- ductor is at +5000 volts, the other at 5000 volts. The circle ( oo radius) midway between is at 0. The potentials in space on the different equipotential surfaces, starting at the positive sur- faces, are +5000, +4500, +4000, +3500, +3000, +2500, +2000, + 1500, +1000, +500, 0, -500, -1000, -1500, -2000, -2500, 3000, -3500, -4000, 4500, -5000. A very thin insulated metal cylinder may be placed around an equipotential surface without disturbing the field. If this conducting sheet is con- nected to a source of potential equal to the potential of the surface which it surrounds, the field is still undisturbed. The original conductor may now be removed without disturbing the outer field. 1 The dielectric lines of force and the equipotential surfaces are at right angles at the points of intersection. The dielectric lines always leave the conductor surfaces at right angles. The equipotential circles have their centers on the line passing through the conductor centers, the dielectric force circles have their centers on the neutral line. Energy does not flow unless these two fields exist together for instance, if the dielectric field exists alone it is aptly spoken of as "static." 1 Plots made by the author and first published in the G. E. Review, Dec., 1914. INTRODUCTION The energy stored in the dielectric field is where e is the voltage and C a constant of the circuit called the permittance (capacity) and the energy stored in the magnetic field is where i is the current and L is a constant of the circuit called the inductance. The energy stored in the dielectric circuit is thus greater for high voltage, and in the magnetic circuit for high currents. When energy was first transmitted, low voltages and high cur- rents were used. The magnetic circuit and magnetic field in this way became known to engineers, but as little trouble was had with insulation, the dielectric field was therefore not generally considered. If insulation broke down, its thickness was in- creased without regard to the dielectric circuit. A magnetic circuit is not built in which the magnetic lines are overcrowded in one place and undercrowded in another place in other words, badly out of balance. Since voltages have become high it is of great importance to properly proportion the dielectric circuit. Although an unbalanced magnetic field may mean energy loss, an unbalanced or too highly saturated dielec- tric field will mean broken down insulation. The dielectric and magnetic fields may be treated in a very similar way. 1 For instance, to establish a magnetic field a mag- neto-motive force is necessary; to establish a dielectric field an electro-motive force is necessary. If in a magnetic circuit the same flux passes through varying cross sections, the magneto- motive force will not divide up equally between equal lengths of the circuit. Where the lines are crowded together the magneto- motive force per unit length of magnetic circuit will be larger than where the lines are not crowded together. The magneto-motive force per unit length of magnetic circuit is called magnetizing force. Likewise for the dielectric circuit where the dielectric flux density is high a greater part of the electro-motive force per unit length of circuit is required than at parts where the flux density is low. Electro-motive force or voltage per unit length l See Karapetoff, "The Magnetic Circuit," and " The Electric Circuit." Steinmetz, "Electric Discharges, Waves and Impulses." 4 DIELECTRIC PHENOMENA of dielectric circuit is called electrifying force, or voltage gradient. If iron or material of high permeability is placed in a magnetic circuit the flux is increased for a given magneto-motive force. If there is an air gap in the circuit the magnetizing force is much greater in the air than in the iron. If a material of high specific capacity or permittivity, as glass, is placed in the dielectric circuit, the dielectric flux is increased. If there is a gap of low permit- tivity, as air, in the circuit, the gradient is much greater in the air than in the glass. The electric circuit is also analogous, as will appear later. A given insulation breaks down at any point when the dielec- tric flux density at that point exceeds a given value. It is thus important to have uniform density. The flux, ^, depends upon the voltage, the permittivity, or specific capacity of the insulation, and the spacing and shape of the terminal. That is, * = Ce The flux density D, at any point, is proportional to the gradient g, or volts per centimeter at that point, and to the permittivity of the dielectric. Thus, D = ^ Kk = gKk dx & also D = j As the density is proportional to the gradient, insulations will, therefore, also rupture when the gradient exceeds a given value; hence if the gradient is measured at the point of rupture it is a measure of the strength of the insulation. The strength of in- sulation is generally expressed in terms of the gradient rather than flux density. By analogy with Hooke's Law the gradient may be thought of as a force or stress, and the flux density as a resulting electrical strain or displacement. Permittivity, fc, then, is a measure of the electrical elasticity of the material. Energy is stored in the dielectric with increasing force or voltage and given back with decreasing voltage. Rupture occurs when the unit force or gradient exceeds the elastic limit. Of course, this must not be thought of as a mechanical displacement. In fact, the actual mechanism of displacement is not known. When two insulators of different permittivities are placed in series with the same flux passing through them, the one with the INTRODUCTION 5 lower permittivity or less electrical elasticity must take up most of the voltage, that is, the "elastic" one may be thought of as " stretching" electrically and putting the stress on the electrically stiff one. The dielectric circuit is also analogous to the electric circuit when the flux is thought of in place of the current and the permittance as conductance. The reciprocal of the permit- tance is sometimes called the elastance ($) and corresponds to " resistance" to the dielectric flux. It is convenient when permittances are connected in series, as the total elastance is the sum of the elastances. When permittances are connected in multiple, the total permittance is the direct sum of the permit- tances. Take two metal plates in air and apply potential between them until the flux density is almost sufficient to cause rupture. Now place a thick sheet of glass between the plates; the permittance and therefore the total flux is increased. This increases the stress on the air, which breaks down or glows. The glass does not break down. Thus by the addition of insu- lation the air has actually been broken down. This takes place daily in practice in bushing, etc., and the glow is called static. It is especially important in designing leads and insulators im- mersed in air to avoid overstress on the air. It can be seen that a statement of volts and thickness does not determine the stress on the insulation. The stress on insulation does not depend altogether upon the voltage, but also upon the shape of the electrodes; as, for instance, for needle points the flux density at the point must be very great at fairly low voltages, while for large spheres a very high voltage is required to pro- duce high flux density. For this reason 200 kv. will strike 55 cm. between needle points, while it will strike only about 17 cm. between 12.5-cm. spheres. From the above it can be seen that it is much more important to design the dielectric circuit for proper flux distribution than the magnetic circuit. Local overflux density in the magnetic circuit may cause losses, but local overflux density in the dielectric circuit may cause rupture of the insulation. Consider now the two conductors of a transmission line with voltage between them. The total dielectric flux begins on one conductor and ends on the other conductor (see Fig. l(d)). The flux is dense at the conductor surface and less so at a distance from the conductor. Hence the voltage gradient is greatest at the surface, where the dielectric cross-section is a minimum, 6 DIELECTRIC PHENOMENA and therefore the "flux resistance" or elastance is greatest and breakdown must first occur there. For the particular case shown in Fig. 2 one-third of the voltage is taken up by the space 12 cm. from each conductor, although the total space is 100 cm. The gradient is greatest at the wire surface. That is, if across a small distance, Xi 9 the voltage is measured near the wire surface and then again across the same space X% some distance from the wire, it is found that the voltage is much higher across the small space Xi near the wire surface than across the one farther out. In ac- tually measuring the gradient, or rather cal- culating it, X is taken very small or dx. The voltage across dx is de. The purely mathemat- ical expression for the gradient at the surface of parallel wires is: +50 -50 de dx q = - . = y j~. 2r FIG. 2. Voltage in space between two par- allel wires. If the conductors are close together a spark jumps across when the voltage is high enough to produce overflux density at the conductor surface; or corona and spark-over are simultaneous. If far apart, corona forms around the conductor surface and sparkover takes place at some higher voltage. As voltages or electro-motive forces become higher the proper shaping and spacing of the conductors to prevent dielectric flux concentration becomes of more importance. The dielectric field must now be considered in the design of apparatus as the magnetic field has been considered. Certain phenomena always exist which go unnoticed because of their feeble effect, but which when conditions are changed, usually in a way to cause a greater energy density, become the controlling features. This is so with the dielectric circuit. The problem first made itself apparent to INTRODUCTION 7 engineers in the transmission line, which will be taken to illus- trate this. When voltages were below about 60,000 the conduc- tors used had sufficient radius or circumference so that the surface flux density or gradient was not sufficient to cause breakdown. As voltages became higher the sizes of conductors remained about the same, and therefore the flux density or gradient became greater. The air broke down and caused the so-called corona and resulting loss. As high voltage engineering problems will be, to a great extent, problems of the dielectric circuit, this will be discussed in the next chapter and calculations made for a few common forms of electrodes. The determination of the dielectric flux density, etc., is purely a mathematical problem. Exact calculations are diffi- cult and often impossible except for simple forms. Exact calcu- lations are not necessary in practical design work, but the general principles must be kept in mind. CHAPTER II THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT If two conductors placed in a dielectric, as, for instance, the two parallel wires of a transmission line in air, are connected together at one end by an electric motor, or resistance and poten- tial is applied across the other end from an a.c. generator or other source of power supply (see Fig. 3), energy transfers take place. The motor at the far end turns and part of the energy is thus used as useful work part appears as heat in the motor. ~TT TTTT FIG. 3 Transmission line carrying energy. As a function of the current in the transmission circuit and a constant called the resistance, energy is absorbed. This energy appears as heat in the conductors; it is proportional to the product of the square of the current and the resistance, and is commonly known as the IV loss. Hence, as it is not returned to the circuit or transferred into useful work, but is dissipated as heat, it is analogous to a friction loss. During the transmission, energy is stored in the space surrounding the conductors in the electric field in two different forms magnetic and dielectric. Energy is stored in the magnetic field, where it is proportional 8 THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 9 to the square of the current and to a constant of the circuit called the inductance: PL Magnetic energy is stored with increasing current and delivered back to the circuit with decreasing current. The magnetic energy becomes noticeable or large when the currents are large, or in low voltage circuits. Due to the dielectric field, the energy is e o-f- \AAA7 W c = This energy is stored with increasing voltage and delivered back with decreasing voltage. A dielectric may thus by analogy be thought of as an electrically elastic material, which is dis- placed by an electric pressure, i.e., voltage. Energy is hence stored in the dielectric with in- creasing voltage or electric pressure, is maximum at the maximum point of the voltage wave and is delivered back to the circuit with decreasing voltage. When the pressure becomes too great the electric u elastic limit 13 is exceeded, or the dielectric becomes dis- torted beyond this "elastic limit," and rupture occurs. The dielectric energy becomes of great importance at high voltage, and hence in the study of insulations, and it only will be considered here. The electric displacement may be pictured in magnitude and direction by lines of force. The dielectric lines of force for two parallel con- ductors are shown in Fig. 3, the eccentric circles (dotted) are the magnetic lines of force. The magnetic circles are also equipo- tential boundary lines for the dielectric field. The dielectric energy is sometimes said to be due to a charge on the con- ductor. This is often confusing, as the energy is stored not AAAA 180 360 lime 540 720 FIG 4. Variation of dielectric and magnetic stored energy with voltage and current. 10 DIELECTRIC PHENOMENA on the conductor but in the surrounding space, and may be thought of as due to an electric displacement. The nature of this displacement is not known. It can be seen that in order that a transfer of energy may take place, energy must be stored in the space surrounding the conductors in two forms magnetic and dielectric. Energy thus flows only in a space in which there is a magnetic and a dielectric field. This energy is proportional to the product of the magnetic and dielectric field intensity and the sine of the included angle. If one field exists alone there can be no energy flow. The change of stored energy from magnetic to dielectric and back is shown in Fig. 4. Dielectric Field between Parallel Planes. In the dielectric field the flux or total displacement is & = Ce coulombs (or lines of force) (1) where e is the applied e.m.f . or voltage, and C is a constant of the circuit, depending upon its dimensions, and is called the capacity, FIG. 5. Dielectric field between parallel planes or better, permittance. If C is measured in farads, and e in volts, \f/ is expressed in coulombs. Fig. 5 shows the simplest form of dielectric circuit. Neglecting the extra displacement at the edges, it is seen that the dielectric lines of force are everywhere parallel and the field is uniform. The dielectric circuit constant, or the permittance, is directly proportional to the area of the cross- section perpendicular to the lines of force, inversely propor- tional to the spacing along the lines of force, and directly propor- tional to the dielectric constant or the permittivity. For large parallel planes without flux concentration at the edges (j = - j I j = Y k K farads (2) THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 11 where A is the area in square centimeters, X is the distance between plates in centimeters, k is the specific inductive capacity, or better, permittivity, and v is the velocity of light, 3 X 10 10 cm., per second. The term in brackets is due to units. The flux density then, or displacement per unit area, as the flux is uniform, is: ~ ^ Ce . , _ /ox j) z_ -. = ~ - coulombs per cm. 2 (3) A A X4:TTV 2 * To establish this flux or displacement through the distance X an electromotive force e is required. The force per unit length of dielectric circuit or electrifying force is constant in the uniform / field and is then ^. The gradient then is g = Y volts/cm. The density may thus be written: which is analogous to Hooke's law in Mechanics, strain = k times stress. The larger k is, the greater the displacement is for a given force g. Thus k is the coefficient indicating electrical elasticity of the material, or its "conductivity" to the flux. The reciprocal of permittivity is analogous to resistivity and has been termed elastivity (a-). The reciprocal of permittance has been termed elastance (S). The dielectric circuit then becomes analagous to the electric circuit volts , e TTE - : ~I - " Or ^ = ~Q flux resistance" 8 It is often convenient to consider the dielectric circuit in this way, and to use Force FIG. 6. Concentric cylinders. The permittance of the condenser of thickness dx, over which the field is uniform (Fig. 6), per centimeter length of cylinder is JQ __ j (1\ fa ^ 7ry _ 2 ^ x ^ TV * ^ 2 fa \C7 "" A" fclO 9 "" 2irx klQ* ~ fclO 9 x r*% R f*x - s* /^a? B I VO/ I A/JLU I *^ ^y a? = r t/ a: = r y a - r 7 j Se __ _ 5.55 fclO~ 13 farads per centimeter ,. ^ 2v* log* R/r ~ loge fl/r length of cylinder. ^ Gradient and Flux Density. The flux density is greatest at the conductor surface and, hence, the gradient must be greatest there. The flux density at any point x measured from the center is --- u " A ~ A "~ A2v* loge R/r A = 2irx . n ek 109 ^ efc - coulombs ' ' D = 10 " - x log, R/r per m. (6) g is maximum at the surface of the inner cylinder or where x = r 14 DIELECTRIC PHENOMENA Parallel Wires. Parallel wires, one of the most common prac- tical cases, will be considered in detail, in order to illustrate the general method of calculating the dielectric circuit and to show that the expressions for the permittance, flux density, gradient, etc., are quite simple and can be written with the aid of ordinary geometry and calculus. Equipotential Surfaces, Lines of Force, and Flux Density. All of the equipotential surfaces which arise in this case are cylin- drical. Therefore, only their intersections with a normal plane need be considered, and the problem may be dealt with as affecting only the plane. Fix. 7. Lines of force between parallel wires, by superposition of independent radial fields. The following principles will be used: (1) The resultant field in the space between two conductors is the superposition of the two independent fields. The re- sultant field due to any number of fields may be found by combining in pairs. Fluxes may be added directly. (2) The potential at any point is the algebraic sum of the potentials due to the independent fields through that point. In the same way, the potential difference between two points THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 15 FIG. 8 (a). Lines of force and equipotential surfaces between parallel wires. FIG. 8(b). Lines of force, equipotential surfaces, and equigradient surfaces between parallel wires. 16 DIELECTRIC PHENOMENA is the algebraic sum of the potential differences due to the independent fields. (3) The density or gradient at a point is the vector sum of the densities or gradients due to the independent fields. When the conductors are infinitely small, the dielectric field may be considered as that resulting from the superposition of the two uniform radial 1 fields from the conductors to an infinite cylinder. The resultant equipotentiai surfaces are then cylinders whose right sections are eccentric circles which enclose the wires, and whose centers all lie in the line connecting them; and the lines of force are arcs of circles intersecting in the conductors. The independent radial fields about each conductor are shown in Fig. 7, and the field resulting by superposition is shown in Fig. 8. FIG. 9. The equipotentiai surfaces will first be considered. It has been shown above that the permittance C between two equipotentiai cylinders of radii R and r is c = 27rfc 5. farads per cm. (5) log* R/r This is also the permittance between any two points on these surfaces; therefore, the voltage between points distant ri and r 2 cm. from the conductor center is e ri/r 8 - Considering now the field resulting from superposition: In 1 By uniform radial field is meant one in which equal central angles always include equal fluxes. THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 17 Fig. 9, the potential difference between H 2 and P, due to the radial flux \l/ from A'i, is Similarly, the potential difference between H% and P, due to the radial flux \l/ from A' 2, is 1 b P2 2irkK The total potential difference between H 2 and P due to the two radial fields, and hence due to the resultant field, is the algebraic sum of the potential difference produced by each field separately: But if H 2 and P are points on the same equipotential surface the potential difference between them is zero, or e p = 2wkK Therefore log e = log e d> o a?i a , = T = const. a? 2 o if jff 2 is fixed that is, for any one equipotential surface. The equipotential surfaces are cylinders whose sections are circles which surround the infinitely small conductors. These circles have centers on line AiA% 9 but are not concentric with the conductors. This may be shown as follows: Assume Cartesian axes through A 7 2 , the X axis containing A'\. Let the coordinates of P be x, y, Xi _ a _ /i to " 6 " \" (a + b - xY + 1 The signs must always be properly placed. It is convenient to give ^ the sign of the point displacement under consideration. The distances from the displacement points to the points between which potential is sought should always be put in the same order in the log, as, Zi/a, x 2 /&, etc. See problems, Case 11 and Case 12, Chap. X. 2 18 DIELECTRIC PHENOMENA ( a 2 _ ( a 2 _ 52)^2 = 5)2 6 V / , & 2 \ V * + c I - 67 (a (a - (7) This is the equation of a circle whose center has the coordinates ^ 2 ab > and whose radius is - r The circle is thus found for 'a-6 T a 6 any given a and 6. The equipotential circle through any point P (x p , y p ) is found as follows: "~a + Z> "" a + b Substituting for a and 6 in (7) : #2 2 + (**} \(xi + g) 2 / > 2 , ' ^ a; 2 2 = + { (8 e - resultant lines of force are arcs of circles with centers on line n and passing through the points A'i and A' 2 . This is shown as follows: Consider Fig. 10. The flux included In PA\ A 1 2 per THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 19 centimeter length of cylinder due to A\ is ~ That in A' i due to A ' 2 is AW The total flux between P and A f i A f % is the sum of these, ^ 2x The restriction that lines of force cannot cross implies that the flux between any two is constant; hence if P move along a flux line, ... _ * ,.. , = const * from which a\ + oj2 = const. Hence: a == TT (ai + 0:2) = const. NOTE The equation of the line of force may also be found by writing the expression for FIG. 10. the flux densities at points and imposing the condition that the component normal to the line of force is zero. This condition defines a circular arc passing through A\ and A 1 2. Choosing as before the point A' 2 as the origin of Cartesian coordinates, the equation of these circles is: (8) where m is the ordinate of the center of any' particular circle. The equation of the line of force through (x, y) is found as follows : Call the center of circle (lines of force) AzO = PO = radius of circle _ wV (8) Through any point (x p y p }. 20 DIELECTRIC PHENOMENA Then (y - XP) 2 + (tfp - m) 2 .= ( + 7/p 2 - S'XP _ lib """ Substituting this value of m in (8) : The slope of the equipotential surface at (x p , y p } is found from (7a). Evaluate T/ in terms of a?, differentiate, and put # = x p . NOTE Take x always + ^ when below x axis. dy__ _ S 7 a? P - ap 2 + yp 2 __ _ fe s yp(S' - The slope of the line of force at (x p , y p ) is found in the same way from (8a) dy y P (S' - S'x P It will at once be noticed that dy _ _ dx e8 dx which shows that the line of force at any point is perpendicular to the equipotential surface at the same point. The flux density, D, at any point in the resultant field is the vector sum of the flux densities due to A\ and A'% separately. At P (Fig. 10) the flux density due to A'i is and due to A\ is 1)2 = directed as indicated. NOTE. Subscript es refers to equipotential surface. Subscript If refers to line of force. THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 21 The triangles whose sides are Xi, x Zj S' and D 2 , DI, D may be shown to be similar, having one angle (a) equal, and the including sides proportional. Then D S' The preceding, covering infinitely small wires, is not directly applicable to the ordinary case of large parallel wires. Green's theorem, however, states that if any equipotential surface be kept at its original potential, the flux within it may be removed without any change in the external field. In Fig. 11 the circles FIG. 11. represent equipotential cylinders, surrounding flux centers A!\ and A'%. These cylinders may be maintained at their original potential. The interior may be filled with a conductor. This gives parallel conductors of radius r and spacing between centers S. The external field has not been changed,. and the preceding discussion still applies. Ai and A 2 must be located from A r i and A '2, since r and S are the quantities given in any actual case. This is easily done: a = S r z b = r - z z = r 2 - 2rz + r 2 - 2rz a b zS = r 2 + * 2 z* - Sz + r 2 = S r z r + z S -2r S - VS* - 4r 2 22 DIELECTRIC PHENOMENA Since obviously z cannot be greater than /S/2, the negative sign is taken for the radical. a = S - T z _ 2>S - 2r - S + VS 2 "^!^ 2 2 = >S - 2r + V 2 - 4r 2 2 6 = r 2 ' = 2r ~ ^ + V>S 2 - 4r 2 2 - 2r + V* - 4r* (1Q) 2r - S + V/S 2 - 4T 2 ^ - 2r + V>S 2 - 4r 2 2r - - Vg 2 "^ " 2r ~ AS + ViS 2 "^ - 4nS + 2(^ ~ 2r) 4r 2 _ (2r -S)(S+ V 2 - 4r 2 ) S 2r(2r -5) Permittance or Capacity. In Fig. 11 let n be a neutral plane. Represent by e n the potential between circle H* and n (or H i and n) and by C n the corresponding permittance to neutral per centimeter length of wires. Due to A'i. Due to 6 , - 6712 "" 2irkK 2-rrkK e n i Xi . a 10g e - loge 5 THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 23 Substituting from (10) C n =^~ 2-TrkK 5.55MO- 13 r , - farads per cm. If hyperbolic tables are available, a more convenient form is C n = o~ cosh- 1 ~ 5.55MO- 1 * , = farads per cm. cosh" 1 ~ 2r If >S/r be large, then^/f -J 1 is nearly equal to H- and approximately (7 = - - -- farads per cm. (lift) loge S/r ^ v J The result corresponds exactly to the form (page 22) which would have resulted had the wires been considered very small at bhe start, or where a = S, b = r Gradient and Flux Density. The flux density at any point on bhe line joining the centers of the conductors and distant x from bhe inner surface of one of them is Xi = a (a + 2ir(ab + (a - tyx - ~ 4r 2 24 DIELECTRIC PHENOMENA - 4r 2 Since = C n e n x) (S - 2r) - 2-n-kKen i r^ log < [a? x)(S - 2r)- a; 2 (S-2r) - 0.885fceuV e corona forms and the voltage must be still further increased be- fore spark-over occurs. This is illustrated graphically in Pig. 12. Note that this is plotted between r/R and g. Thus the minimum occurs when r/R = l/. It is interesting to note here that with a given R a cable has maximum strength when r is made such that R/r This is not the practical ratio however, as will appear later. -i | t-H \ I I 1 I I .1 .2 .3 .4 .5 .6 .7 .8 .9 1.0 r FIG. 12. Concentric cylin- ders. Variation of gradient at surface of inner cylinder as radius is changed outer cyl- inder constant. THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 29 COLLECTED FORMULA FOR THE COMMON ELECTRODES Concentric Cylinders. : n r 5.55/clO- 13 . , Capacity C = , ^n farads per cm. lOge jKt/T S) Gradient g x = , =57- kv. per cm. x log, R/r K a Max. gradient g = ~~, =y- kv. per cm. Corona does not form when R/r< 2.718 x = distance from center of cylinder in cm. R = cm. radius of outer cylinder. r = cm. radius of inner cylinder. Parallel Wires. : Capacity or permittance to neutral 5.55fclQ- 13 5.55fclO~ 13 , , C n = ^ ,... _ = ^ farads per cm. Gradient (at x cm. distance from wire surface on line through centers) __ _ e n \/S 2 4r 2 _ kv. per cm. Max. gradient (at conductor surface) l a = F -i or y ,& ^ r a i . rv . A i r (*r- k - kv. per cm. Corona does Dot form when S/r < 5.85 1 See same equations in different form, page 24. See formula 12c, page 25. 30 DIELECTRIC PHENOMENA S spacing between conductors centers in cm. r = conductor radius in cm. e n = kv. to neutral. Equal Spheres in Air. Gradient (non-grounded). (At a centimeters distance from sphere surface on line joining centers.) _ a) '(/-!)] -4(^-0) (/-I)] 2 kv. per cm. Max. gradient (non-grounded) ~/kv. per cm. Max. gradient (one grounded) g g = - / kv, per cm. where / = + 1 + (Z/fl + 1) + 8 4 and /o = see table, page 27. Corona does not form when X/R < 2.04 R = radius of sphere in cm. X = cm. spacing between nearest surfaces. e = kv. bet. spheres. Capacity or permittance farad, 3601) Combination of Dielectrics of Different Permittivities. When several dielectrics of different permittivities are combined, as is usually the case in practice, it becomes important to so proportion and shape the electrodes and insulations that one dielectric does not overstress another. This is of especial importance in insu- lators where dielectrically weak air of low permittivity is neces- sarily in combination with dielectrically strong insulations of high permittivity. Dielectric Flux Refraction. When dielectric flux lines pass from a dielectric of permittivity fci to another of permittivity of fcz the lines are bent or refracted. This does not occur, of course, THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 31 when the lines strike the surfaces normally, as in a concentric cable, and between parallel plates already considered. The angle of refraction bears a definite relation to the ratio of the two permittivities and can be shown as follows: Let AB, Fig. 13, be the common surface of the two insulations. The flux ^i makes an angle i with the normal NN to the sur- face. The total flux through the equipotential surface ab is the same as the total flux through the surface cd. The voltage be- tween a and c must be the same as the voltage between b and d, because potential at a = poten- tial at b and potential at c = po- tential at d. Therefore $ = Di ab = In the uniform field (14) FIG. 13. Dielectric flux refraction. e bd where e is volts, a to c = volts b to d Therefore gibd = g z ac Combining (14) and (15) Di ab Dz cd But = KI D 2 /02 = (15) Therefore Therefore tan 4>i tan i tan 02 tan 02 Dielectric in Series. Take the simple case of two parallel planes with two different dielectrics between them and neglect the flux concentration at the edges (Fig. 14, flux concentration not 32 DIELECTRIC PHENOMENA shown). As the lines are normal to the electrodes there is no refraction. The same flux passes from plate to plate. C 2 = 61 e = ei + TT i ^ t -* - l- h " 1 \ \ 1 U! _ ki '' FIG. 14. Dielectrics of different permittivities in series. The voltages are therefore divided thus e /I + ^i The gradients are (16) The voltages and gradients may be found in the same way for any number of insulations in series. The expression for the gradi- THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 33 ent at any point in a combination of n insulations in series is: e_ ^^ Where the distance between the electrodes is greater than the radius of the edges the increase in stress at the edges becomes appreciable. Concentric Cylinders. For concentric cylinders the expression may be found in the same way. The flux lines in this case also are normal at every boundary surface and are hence not refracted. Consider a wire of radius r\ surrounded by n insula- tions whose inside radii are respec- tively 7*1, r 2 , . . . r n , and whose per- mittivities are &i, fc 2 , . . . k n . At the distance x from the center of the wire, which falls in the dielectric of inside radius r x , outside radius r x+ i, nd permittivity k x , the expression for FlG - 15 * he gradient g x is found as follows: fC = 1/Ci + 1/C* + . . .+1/C.+. . . +1/C _ 1 /log* r 2 /ri L og e r 3 /r 2 loge (r a + l)/ra. 2?TjK \ ki A/2 1 1 ^, 1 , log e R/r n \ " " k n ) f r jr 1 ~" K /log*. r 2 /ri r lo&rs, /r 2 , , log^+yr* , A log e R/r n \ \ fci ' fci T-- - - 1 7 t - - 1 r, / tug fun > D "-Z Ce * "A 27TjK 6 ~ 27TO; /Iog e r 2 /ri Iog e r 3 /: 7*2 , , loge T x+1 /r a . . loge jR/7*n\ V fci fc 2 n/ar K>n ' ^ = *i (17) 1 6 xk x /Iog e r 2 /ri Ioger 3 /r : 2 , , logeTx+t/rx , , log fi S/r n \ _ __L_ _J. v ! . 1 _ _ _ -4 - _ ' " 1 \ Jbi fca *. 34 DIELECTRIC PHENOMENA FIG. 16. The refraction of lines of force passing through a porcelain insulator (permittivity assumed 4). FIG. 17. Dielectrics in multiple. FIG. 18. Rod and ring with two di- FIG. 19 Dielectrics in multiple electrics. Boundary of dielectrics and in series. along line of force. (Not drawn to scale.) Dielectrics in Multiple. Where dielectrics are combined in multiple, the division between the dielectrics being parallel to the lines of force (Fig. 17), the stress on either is the same as it THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 35 would be were the other not present. Fig. 18 shows a rod in- sulated from a ring by a dielectric so shaped as to make use of this fact. Where the division line is not parallel to the lines of force, some lines must pass through both dielectrics (Fig. 19). For these lines the insulators are in series, and the corresponding precautions are necessary, just as in Fig. 14. -IOOK.V. .^Isolated OK.V, FIG. 20. Field not changed by a thin insulated metal plate on an equi- potential surface. Flux Control. In certain electrical apparatus it is very often possible to prevent or reduce dielectric flux concentration by superposing fields upon existing fields. When it is necessary to Superpose two fields, as often happens in the course of design, it is important to see that it is properly done. For instance, as a simple case, suppose the two plates. A and B in Fig. 20, are at (a) (6) 50K.V 50K.V. OK.V. OK.V A FIG 21. (a) Field not changed if the potential of the plate is the same as that of the surface upon which it rests, (b) Field changed by plate at potential different from the surface. potentials of and 100 kv. respectively. A thin insulated metal plate, C, may be placed anywhere between A and B without changing the field as long as it follows an equipotential surface that is, parallel to A and B. Unless it follows an equipotential surface flux concentration results. If C is insulated and brought to a potential of 50 kv., the field will be disturbed unless C follows the 50 kv. equipotential surface, or, in other words, is midway 36 DIELECTRIC PHENOMENA between the two plates otherwise the stress in part of the in- sulation will be greatly increased. See Fig. 21 (a) and (6). Fig. 21 (a) shows the position for no change. Fig. 21(6) shows very great increase of stress on part of the insulation. A coil of wires in which the turns are at different potentials may be placed in the field with least disturbance if the potential of each coil corresponds to the potential of the equipotential surface upon which it rests, as shown approximately in Fig. 22 (a). (6) i -80 Mil I - - f *\ ~ - -. - -60 10 " (f)i \ ) \ r --20 ' - A ffVl 100 K.V, OK.T. FIG. 22. Conductors placed in a uniform field. When insulation is used around small conductors, points, etc., the stress may be very great. This stress may be reduced by superposing a uniform field. For instance, take two small paral- lel wires with voltage e between them, the stress is 9 = 2r log e a If a uniform field is superposed, as in Fig. 22(6) of gradient gi ~> the stress on the wires becomes These principles must be used in generator and transformer design, etc., and will be applied in a later chapter. Imperfect Electric Elasticity. The electric displacement has been shown to follow Hooke's law by analogy, that is, Ce or D - strain == constant X stress. The dielectric has so far been assumed to be perfectly elastic. For a perfectly electrically elastic material C or k must be con- THE DIELECTRIC FIELD AND DIELECTRIC CIRCUIT 37 stant and independent of the time that the stress e or g is applied. This appears to be the case for perfectly homogeneous dielectrics as air, various gases, pure oil, etc., but" is not so for non- homogeneous dielectrics. As an example of imperfectly elastic dielectrics take a cable; when potential is applied between core and case the displacement immediately reaches very nearly its full value, but gradually increases through an appreciable time slightly above its initial value. It thus appears that energy is slowly absorbed and this phenomenon has, therefore, been termed absorption. When the above condenser is disconnected from the supply, and then short circuited, the potential difference becomes zero. If the short circuit is removed a very small potential difference gradually reappears as residual. If such a condenser is displaced (charged), and the supply is removed, the displace- ment gradually disappears by conduction or leakage. In meas- uring the high voltage d.c. resistance of cable insulation it is often necessary to allow several minutes to elapse before the current becomes constant. The residual is analogous to residual stretch in an imperfectly elastic metal wire. For instance, if a steel rod is stretched and the stress is removed, it immediately assumes very nearly its initial length, but there is always very small residual stretch which very gradually disappears. It has been shown theoretically that the phenomenon of ab- sorption should exist for non-homogeneous dielectrics, but not for homogeneous dielectrics. In non-homogeneous dielectrics the effect of this residual is to cause the flux to lag behind the voltage if the voltage change is rapid as in the case of high frequency. This is analogous to damping. If the change in voltage is slow, however, the effect would not result. A loop may thus be plotted (when the change of voltage is rapid) between voltage and displacement, similar to the hysteresis loop. If the frequency is very low or the dielectric is homogeneous the loop does not result. This loop means loss, but it is not analogous to hysteresis loss in iron which is independent of time. CHAPTER III VISUAL CORONA SXJMMAKY Appearance. If potential is applied between the smooth conductors of a transmission line or between concentric cylin- ders and gradually increased, a voltage is finally reached at which a hissing noise is heard, and if it is dark, a pale violet light can be seen to surround the conductors. This voltage is called the critical visual corona point. If a wattmeter is inserted in the line a loss is noticed. The loss increases very rapidly as the vol- tage is raised above this point. The glow or breakdown starts first near the conductor surface, as the dielectric flux density or gradient is greatest there. As the broken down air near the surface is conducting, the size of the conductor is, in effect, increased by conducting corona. This increases for the given voltage until the flux density or gradient is below the rupturing gradient, when it cannot spread any more. If the conductors are very close together, a spark strikes between them immediately and corona cannot form. If the conductors are far apart corona forms first, and then, if the voltage is sufficiently increased, a spark strikes across. Whenever corona is present there is always the characteristic odor of ozone. Air consists of a mechanical mixture of oxygen (Oa) and nitrogen (N). When air is overstreSsed electrically the oxygen molecule is split up into O, when it becomes chemically very active. The atoms again combine by the law of probability O into O = O, (O 2 ), the normal state, and /\ > (O 3 ) or ozone. Oxygen in the nascent state (O) also combines with metal, organic matter, etc., if such are present. Ozone is also not stable and is, hence, chemically active; it splits up as O2 and O when the latter combines readily with metals, and organic matter. If the electrical stress is very high the oxygen enters into chemical combination with the nitrogen, forming oxides. The energy loss by corona is thus in a number of forms, as heat, chemical action, light, noise, convection, etc. A.C. and D.C. Corona. When alternating voltage higher than the critical voltage is applied between two parallel polished wires, 38 FIG. 23. A. C. corona on polished parallel wires. -f FIG. 24. Corona on parallel wires. Iron. First polished and then oper- ated at 120 kv, for two hours to develop spots. Diameter, 0.168 cm. Spacing, 12 . 7 cm. Stroboscopie photo., 80 kv.-60 ~. (Facing page 38,) Wire "dead". FIG. 25. D, C, corona on smooth wires by Watson. (See Fig. 79.) VISUAL CORONA 39 the glow is quite even, as shown in Fig. 23. After operation for a short time reddish beads or tufts form along the wire, while around the surface of the wire there is a bluish-White glow. If the conductors are examined through a stroboscope, so that one wire is always seen when at the positive half of the wave, it is noticed that the reddish tufts or beads are formed when the con- ductor is negative and the smoother bluish-white glow when the conductor is positive. (See Pig. 24.) A.c. corona viewed through the stroboscope has the same appearance as d.c. corona. (See Fig. 25, d.c. corona.) The d.c. corona on the + wire has exactly the same appearance as the a.c. corona on the + half of the wave; the same holds for the wire. Measure of Stress. The gradient in kilovolts per centimeter is a measure of the stress on the dielectric. For parallel wires the gradient at the wire surface, and hence where the stress is a maxi- mum and where the "dielectric elastic limit" is first exceeded, is de __ _ e dx ~~ g ~ r log e S/r That is, if the voltage between the surface of the conductors and a point in space at infinitesimal distance dx cm. away is de t then this gradient in the limit at the surface is de __ _ e dx ~~ ~~ r loge S/r If e is e v , the observed voltage to neutral at which visual corona starts, g v is a measure of the stress at breakdown. For a wire in the center of a cylinder * r log, R/T Influence of Wire Spacing and Diameter on Apparent Strength of Air. If the visual corona voltages are measured for a given conductor at various spacings, it is found that #, or the apparent strength of air, is a constant independent of the conductor spacing. It would also naturally be expected that g v would be a constant for all conductors independent of their diameter, or in other words, air would break down under the same constant unit stress inde- pendent of the size of the conductor; just, for instance, as differ- ent sized rods of the same material would be expected to break down at the same unit stress of kilograms per square centimeter. It has long been known, 1 however, that air is apparently stronger at 1 Ryan, The Conductivity of the Atmosphere at High Voltage, A.I.E.E., Feb., 1904. 40 DIELECTRIC PHENOMENA the surface of small conductors than large ones. (The measured apparent strength curve is given in Fig. 28.) Of course this does not mean the voltage required to start corona is greater for small wires than for large ones (it is lower for the small conductors at a given spacing), but that the term g V} or unit stress in the expression e = g v r log* S/r is greater for air around small conductors than large ones. This apparently greater strength of air around small conductors was long attributed to a film of condensed air at the conductor surface, because such a film would have a greater relative effect for the smaller conductors. We have given another reason for this which experiments at low air densities seem to confirm. During our first investigations we found that the relation between the apparent strength of air and the radius of the conductor could be expressed by the simple formula + ~~ J (18) where g is a constant and is about 30 kv. per centimeter. 1 This means that the stress at the conductor surface at breakdown is not the same for all diameters, as already stated, but always constant at a distance 0.301-v/? cm. from the surface. (See Fig, 29.) This follows: 0.301 \ _ r loge S/r e>... therefore, g = (r + 0-801 loge s/r The gradient x cm. from center of the conductor is approxi- mately - X lOge S/T x = ( r therefore, g is the gradient 0.301-\/r cm. from surface. There- fore, by substitution also / 0.301 \ e v = 30 f 1 + ~7^~ r 1& S/r max. kilovolts to neutral or for a sine wave e v = 21.2(1+ ' /- }r log* 8/r kilovolts effective to neutral (19) \ V r J 1 F. W. Peek, Law of Corona, A.I.E.E., June, 1911. VISUAL CORONA 41 The visual corona voltage for any diameter of wire at any spacing may thus be calculated. The explanation seems to be this: Air has a constant strength g for a given density, but a finite amount of energy of some form is necessary to cause rupture or to start corona. It is obvious that this definite, finite energy is necessary, as evinced by appear- ance of heat, that higher transient voltages are necessary, etc. This will be more fully discussed later. Hence the stress at the conductor surface must exceed the elastic limit g 0j or be increased to g v in order to supply the necessary rupturing energy between the conductor surface and finite radial distance in space away (0.301-v/? cm.) where the stress is g , and breakdown occurs. Application of the Electron Theory. The electron theory may also be applied in agreement with the above. Briefly: When low potential is applied between two conductors any free ions in the field are set in motion. As the potential and, therefore, the field intensity or gradient is increased the velocities of the ions increase. At a gradient of g = 30 kv./cm. (5 = 1) the velocity of the ions becomes sufficiently great over the mean free path to form other ions by collision with molecules. This is the property of the negative ion or electron. This gradient is constant and is called the dielectric strength of air. When ionic saturation is reached at any point the air becomes con- ducting, and glows, or there is corona or spark. Applying this to a wire in the center of a cylinder: When a gradient g v is reached at the wire surface any free ions are acceler- ated and produce other ions by collision with atoms or molecules, which are in turn accelerated. The ionic density is thus gradually in creased by successive collisi ons until at .301 -\fr cm. from the wire surface, where g = 30, ionic saturation is reached, or corona starts. The distance OJSOl-v/r, cm. is of course many times greater than the mean free path of the ion and many collisions must take place in this distance. Thus, for the wire, corona cannot form when a gradient of g is reached at the surface, as at any distance from the surface the gradient is less than g . The gradient at the sur- face must, therefore, be increased to g v so that the gradient a finite distance away from the surface, 0.301\/r cm., is g . This is the same as saying that energy is necessary to start corona, and TYlV^ this energy is the S-jr- of the energy of the moving ions necessary to produce ionic saturation. 42 DIELECTRIC PHENOMENA Very Small Spacings or Films. If conductors are placed closer together than this necessary free accelerating or energy storage distance, Q.301V?" cm., the rupturing force or gradient must be increased. This will be better illustrated by later experiments, in which at small spacings air has been made to withstand gradi- ents as high as 200 kv. per centimeter. Air Density. Thus far the discussion has been limited to air at a constant density, or, in other words, constant pressure and temperature. The above energy explanation can be still further checked by considering air at different densities. The value of g given is for air density at sea level (25 deg. C., 76 cm. barom- eter). This has been taken as the standard, or for the density factor 8 = 1. Air at other densities, due to change in tempera- ture and barometric pressure, is expressed as a fraction of this. The relative density for any temperature Or pressure is , 3.926 273 + t For instance, if the temperature is kept at 25 deg. C. and pressure is reduced to 38 cm. 3 92 X 38 ~ 273 + 25 """ " or 1/2 atmosphere. As the air density, or 5 is decreased, the air is less able to resist the electric stress at the increased molecular spacing. Theoretically the strength of the air g in bulk between parallel planes should decrease directly with 5. g = 305 g vj however, the apparent strength of air in a non-uniform field, if the energy theory is true, cannot decrease directly with 5: the energy storage distance should be 0.301V70 (5), or the com- plete expression should take the form A , 0.301 = 005 1 + Vr We have found experimentally that the energy storage distance a = 0.301 ~ cm.; that is, g v = 305( 1 ~~ V5 \ V5r/ The electron theory may also be applied here: VISUAL CORONA 43 g , the strength of air, varies directly with 5. g v , however, cannot vary directly with 6 because with the greater molecular spacing or mean free path of the ions at lower air densities, a greater " accelerating" distance is necessary in the equation a = 0.301 A/r/S that is, "a" increases with decreasing 5. This is shown experimentally by sphere gap tests. For parallel planes r = < . " . g v = g 5, as expected. The equation for the visual critical corona voltage may now be written: / 0.301 \ e v = g v dr log e S/r = g M 1 + ~-y= Jr log e S/r kv. (20) where e v is Kv to neutral. g = 30 for max., g = 21.1 for effective sine wave. It may be of interest to note that with a pair of smooth wires, of a known diameter, high voltages may be accurately measured anywhere by noting the spacing at which corona starts, the tem- perature and barometric pressure, and substituting in the above formula. The various other factors affecting visual corona will be mentioned. Conductor Surface Cables Material. For rough or weath- ered conductors corona starts at lower voltages. This is taken care of by the irregularity factor, m v . For cables and weathered wires the complete formula becomes e v = m v Bg v r log, S/r For the same surface condition the starting point is independent of the conductor material. Oil and Water, Current in the Conductor, Wave Shape, Etc. Water, sleet and snow lower the visual corona voltage. Oil on the conductor surface has very little effect. Humidity has no effect upon the starting point of visual corona. Initial ionization over a considerable range has no appreciable effect at commercial frequencies. Current in the wire has no effect except that due to heating of the conductor and surrounding air. Wave Shape. The corona point at commercial frequencies depends upon the maximum value of the wave. When results are given in effective volts a sine wave is assumed. With peaked wave, corona starts at a lower effective voltage than with a 44 DIELECTRIC PHENOMENA Shield for Small Wire Shield for Large Wire flat-top wave. D.c. corona starts at a value corresponding to the maximum of the a.c. wave or 41 per cent, higher than the effective a.c. critical voltage. 1 See appendix for further data. The above summary will now be taken up more in detail and experimental proof given. EXPEKIMENTAL STUDY OF VlSTJAL CORONA Effect of Spacing and Size of Conductor. The visual critical voltage, or voltage at which visual corona starts on polished conductors of a given diameter and spacing, at con- stant air density, can be repeat- edly checked within a small per cent. Visual tests were made on two parallel polished con- ductors supported indoors on wooden wheels in a wooden framework. The wires were not allowed to come directly in contact with the wood but rested on aluminum shields. (See Fig. 26.) The object of the shields was to prevent the glow at low voltages which would take place if the wires came in contact with the wood. The tests were made in a dark room, and method of procedure was as follows: Conductors of a given size were placed upon a framework; voltage was applied and gradually increased until O o o O FIG. 26. Wire support for visual corona tests. the visual critical corona point was reached. Critical points were taken at various spacings and recorded as in Table I. Unless otherwise stated tests were made at 60 ~. As the visual critical voltage, e v , is the voltage at breakdown of the air, the surface gradient corresponding to this voltage must be the stress at which air ruptures. This is called the visual critical gradient g v . Where the wires are far apart or S/r is large de e v dr r loge S/r 1 Peek, The Effect of High Continuous Voltages on Air, Oil and Solid Insulation, A.I E.E , June, 1916. VISUAL CORONA 45 where e v = the (maximum) voltage to neutral r = radius of the conductor in cm. S = distance between centers of conductors in cm. Values of gradient calculated for a given conductor at various spacings are given in Table I. (See Fig. 27.) It is seen that the breakdown gradient is constant, or independent of the spacing. This test was repeated for various diameters. The values of the gradients are tabulated in Table II and plotted in Fig. 28. ^100 4 80 5 7ft * * O en "3 o "s 50 100 2 5 1C Spacing- S- cm O Badius of Outer Cylinder - R - cm (a) FIG. 27 (a). Variation of visual critical gradient with spacing. (Parallel wires. Diameter constant = 034 cm.) (6) PIG. 27 (b ) . -Variation of visual crit- ical gradient with radius of outer cyl- inder. (Concentric cylinders. Diam- eter of inner wire constant =0 118 cm. ) TABLE I. VISUAL CRITICAL VOLTAGES AND g v WITH VARYING SPACING AND CONSTANT DIAMETER (Polished Parallel Copper Conductors Diameter 0.0343 cm. 60 <^) 9 cm. et. 1 kilovolts between con- ductors (effective) eu 1 kilovolts between con- ductors (maximum) g* kv /cm (maximum) 2.54 12.1 17.0 99.5 2.93 12 4 17.4 99.0 3.18 12 5 17.7 98.5 3.81 13 18.4 99 4 45 13.5 19 99 5 5 08 13 8 19 4 100 5.73 14.0 19 8 99 7.62 14 5 20 5 99.0 15 2 16 22 6 - 97 2 30. 5 17.7 25 97.2 45 6 18 7 26 3 96.1 61. 19 4 27.4 98 106 8 20.6 29 Average, 97 2 99 46 DIELECTRIC PHENOMENA TABLE II. VARIATION OF g v WITH DIAMETER OP CONDUCTORS (Average Values for Polished Parallel Wire 60 ~. Corrected to 25 deg C 76 cm Barometric Pressure) Diameter, cm de 3J-0- kv/cm (maximum) Material Diameter, cm de Tr~ 9 * kv /cm (maximum) Material 0196 116 Tungsten 2043 59 Copper 0343 99 Copper 2560 57 Aluminum 0351 94 Copper 3200 54 Copper 0.0508 84 Aluminum 3230 50 5 Copper 0577 82 Aluminum 5130 49 Copper 0635 81 Tungsten 0.5180 46 Copper 0780 76 Copper 6550 44 Copper 0813 74 Copper 8260 42 5 Copper 1637 64 Copper 9280 41 Copper 1660 64 Iron JLZU 110 100 |90 |80 I 70 ^60 K CQ ' \ Visual Critical Gradient Two Parallel Wires ^sat 76 am S and 25 V - 29 8 f 1 + .801 *) ff v = Yoltage Gradient k^/an = ^r '' * \ s x^ fts * S 40 - < "-* B ^ -**. . -0 _ "P "" " " >\ I"!.-- = 30 ^o .J) J .2 .3 .4 .5 6 .7 .8 .9 10 11 12 13 14 15 16 17 18 1920 Diameter la cms FIG. 28. Variation of visual critical gradient with size of wire. The gradient at breakdown at the conductor surface is not constant with varying diameters, but increases with decreasing diameters of conductors in other words, air is apparently stronger at the surface of small wires than large ones. The apparent increase in the dielectric strength of air surround- ing small conductors was explained some years ago as due to a condensed air film at the surface of the conductor. If this were so, a higher critical gradient would be expected for tungsten than for aluminum. That is, the air film should be denser around the VISUAL CORONA 47 denser metals. These experiments show that the gradient is not affected by the material or density of the conductor. Ryan 1 has also explained the apparent increase by the electron theory. The explanation first offered in Law of Coronal, 2 and already outlined in this chapter, will now be given more in detail : Assume that air at a given density has a constant strength g , but that a finite amount of energy, be this energy the 2 ^- of the moving 2i ions or whatever form it may, is necessary to cause rupture or start corona. Then the stress at the conductor surface must exceed the elastic limit g , or be increased to g v in order to supply the rupturing energy between the conductor surface and a finite radial distance in space where the stress is g and breakdown occurs, or, in other words, a finite thickness of insulation must be under a stress equal to, or more than g . Just before rupture occurs the gradient at the conductor sur- face is "' - r (21) the gradient a cm. away from the surface is (22) Theoretically, one is also led to believe a = ^ s ' (23) It now remains to test this out experimentally and find The equation of the experimental curve is found to be : = 29 81 + - (24) Substituting (24) in (21) , o^I\ . Vr ) ~ rlo&S/r (r + O.SOIV^) loge S/T Thus the experimental values bear out the above theory a = (r) = O.SOlVr g = 29.8 = constant 1 A I.E.E., January, 1911. See also papers by Whitehead, A I.E.E., June, 1910, 1911, etc. 'A.I.EE., June, 1911 48 DIELECTRIC PHENOMENA That is, at rupture the gradient a finite distance away from the conductor surface, which is a definite function of r, is always constant. (See Fig. 29.) g v = 29.81 V r kv. per cm. A similar investigation made on wires in the centers of metal cylinders (see Figs. 27 and 30) shows as above that the visual <81/r PIG. 29. g v and g<> lor small and large wires. critical gradient, g v , increases with decreasing radius r, of the wire, but is independent of the radius R, of the outer cylinder. The relation between r and g v is given in Table V. For a wire in the center of a cylinder the gradient g is slightly higher than for similar parallel wires, apparently due to the fact that the field is everywhere balanced for a wire in the center of a FIG 30. Apparatus for determining, the visual corona voltage m con- centric cylinders. cylinder, which is not the case for parallel wires. The expression for the apparent strength of air for a wire in the center of a cylin- der is Q1 /- , 0.308 \ . g v 31( 1 H j=- kv. per cm. V V r ] It thus seems that g c = 31 is the true dielectric strength of air. VISUAL CORONA The method of reducing the results to equations was as follows: Various functions of r and g v were plotted for parallel wires from Table II, until it was found that a straight-line law obtained between g v and 1/V^\ All values of g v and l/\/r were then tabu- lated as in Table III and plotted as in curve (Fig. 31). Points 120 .100 20 Vibual Critical Gradient Method of Redacmg Belatio: between ff n and ~ 012345, 678 9 10 FIG. 31. Relation between g v and T=" Vr TABLE III. RELATION OF VISUAL CKITICAL VOLTAGE GEADIENT TO RADIUS (Experimental Values Corrected to 76 cm. Barometer and 25 deg. C. Parallel Wires 60 ~) | Qv i 1 Diameter, kv /cm Radius, V'r Diameter, kv /cm Radius, Vr* cm. (max.) r = cm. cm cm. (max.) r *= cm cm 0.0196 116.0 0.0098 10.10 202 59.1 0.101 3 13 0.0343 99.0 0.0172 7.65 257 56.7 0.128 2 76 0.0350 94.0 0.0175 7.58 0.320 54 3 0.160 2 51 0.0508 84.0 0.0254 6.27 0.322 49.6 0.161 2 51 0.0577 81 5 0.0288 5.90 0.513 48 8 0.256 2.01 0:0635 81.0 0.0317 5.64 0.518 44.5 0.259 1 94 0.078 76.0 0.0390 5 08 0.655 43.7 0.327 1 82 0.0813 73.5 0.0406 4 96 0.826 42 2 0.413 1 57 0.1635 63.8 0.0818 3.51 0.928 40 6 0.464 1 44 0.1660 63.4 0.0830 3 45 varying widely from the average straight line were then discarded as probably in experimental error. The remaining points were then divided into two equal groups and tabulated as in Table IV. 50 DIELECTRIC PHENOMENA TABLE IV. RELATION OF g v AND ~ Vr (Showing 2A Reduction) 1 l g v Vr gv Vr 99 7 65 59 3 13 82 5 90 54 2 51 81 5 64 50 5 2 51 76 5 08 49 2.01 74 4 96 41 1.44 2412 229.23 2253.5 211 60 158.5 = 665.5 158.5 9.00 A2 17.63 22 = = 40.83 Vr 17.63 665.5 - (9 X 40.8) Therefore: 29.8 -f 10 9 29.8 29.8 1 + 0.301 VrJ In order to give proper weight to the points the SA method was used in the evaluations of the constants for the equation above. This method of reduction, which is self explanatory, is very convenient and especially suitable where a large number of experimental points have been obtained, in which case the results are as reliable as, or more so, than when few points are taken and the unwieldy method of least squares used. Temperature and Barometric Pressure. The density of the air varies directly with the pressure, and inversely as the absolute temperature. In these investigations the air density at a tem- perature of 25,deg. C. and a barometric pressure of 76 cm. has been taken as standard. If the air density at this temperature VISUAL CORONA 51 and pressure is taken as unity, the relative density at other tem- peratures and pressures may be expressed in terms of it, thus: 0.004655 w = 273 +t where w = the weight of air in grams per cubic centimeter 6 = barometric pressure in centimeters t = temperature in degrees centigrade. At 25 deg. C. and 76 cm. pressure 0.00465 X 76 AAA110K 25 - 76cm = 273 + 25 = - 001185 S rams w at any other temperature and pressure is 0.004656 ** - 27T+1 wtb 0.004656 3.926 w*s 76cm. ~ (273 + 00.001185 273 + t 3.926 8 ~ (273 +0 On the theory that definite energy is necessary to start dis- ruption or glow, g should vary directly with the air density factor 6; g v , however, should not vary directly with 6, as the thickness of the energy or ionizing film should also be a function of 8. The equation for g* should take the form (25) Whether 6 is varied by change of temperature or air pressure the effect should be the same as long as the temperature is not so high that the air is changed or affected by the heat, as ioniza- tion, etc. Temperature. A series of experiments on visual corona was carried on over a temperature range of 20 deg. C. to 140 deg. C. The apparatus is shown in Fig. 30. It consists of a polished wire in the center of a brass cylinder. The cylinder was placed hori- zontally in a large asbestos lined "hot box," heated by grids at the bottom. In order to get uniform temperature the cylinder was shielded, and time was allowed to elapse after each reading. Temperature was observed by a number of thermometers dis- tributed in the hot box. 52 DIELECTRIC PHENOMENA TABLE V. RELATION OF VISUAL CRITICAL VOLTAGE GRADIENT TO KADIUS (76 cm Barometer 25 deg C Concentric Cylinders) Radius a c R do 1 a c R dc r cm. kv /cm (max ) cm ffv kv /cm r cm kv /cm (max ) cm 0v kv /cm xo CD 059 70 4 10 69 327 48 1 CO 42 0.103 60 7 CO 59 5 476 44 9 JS 39 127 129 58 4 56 6 I 55 5 54 5 794 953 41 9 41 2 O5 00 00 190 52 7 1Q 49 5 1 113 39 7 3 81 f 199 52 7 ; 3 0v (max.) ff'v (max ) 41 -13 75.5 1 139 49 6 50 40 75.5 1.084 48 3 48 37 20 74 9 1 001 44 8 44 9 35.7 41 75 5 0.942 43 2 42 7 33 2 70 75.5 0.863 40 1 39 7 31.5 87 75.5 823 38 1 38 1 29 5 121 75.5 753 35 7 35.4 28 7 130 75.5 0.734 34 7 34 7 Columns 1, 2 and 3 give observed values, surface of the inner cylinder is e The gradient at the 9 = T log e R/T Column 5 gives the surface gradient for the voltage, e v , calculated directly from observed values. It can be seen from the data, that g* for a given r, varies with 5, but is independent of R or S. By 2 A reduction of %11 of the data the following equations connecting g v with r and d were obtained: u 80 60 7 5 K t> 10 ect c fj S C *^ -- ~* <^" -< *** " ^> [o ^ ^-^ ,^- 1 ^ *""* & *** *** -^ *** * .*" X 5^ *-- ^ jt^" *-*f *~* f ^^ at . -" ,- ~~*r - " *~~ * , --^ p These Cut between Therefore ) ; ves show Straight Line Relation 0v and *^y far Oooxatant 5 atgiYen5:-#-y* s fi r o (l+ Vr) .5 1.0 1.5 2.0 2.5 3.0 8.5 4.0 Vfc f temperature on the strength of air. X measured values. For Concentric Cylinders. = 315 1'l + 0.308\ kv. per cm. max, (25a) 54 DIELECTRIC PHENOMENA For Parallel Wires. g v = 29.85 ( 1 H '-?=-} kv. per cm. max. V V5r / (256) M*50 40 .9 1.0 1.1 1.2 1.3 FIG. 33. Effect of temperature on the strength of air. (r = radius of wire in era. X measured values. Drawn curves calculated.) Referring to the tables, column 6 gi^es values of g v calculated from equation (25a). By comparing with the experimental values in column 5 it is seen that the difference is generally less than 1 per cent. 90 80 1 70 I 60 50 M 40 20 Je^Ex^ t> >n "1 ^ ? J^ ^ L^' J^ t^- ^. CV- ^ ^ ^ ^" <* r x ^ ^ ^ r^** r-^ *-" t '"^ ^ / X ^ ^ f ^ in / ^X ^ ^^ Q ^ x^* 1 V .1 .2 .3 .4 .5 .6 .7g.8 .9 1.0 1.1 1.2 1.3 1.4 FIG. 34. Effect of temperature on the strength of air. (X measured values. Drawn curves calculated.) QO has a slightly higher value for wires in a concentric cylinder than for parallel wires. This does not mean that the strength of air differs in the two cases. For a wire in a cylinder the field is balanced all around and should give more nearly the true value. VISUAL CORONA 55 In Figs. 32, 33 and 34 the drawn lines are the calculated values, while the crosses are the observed values. Barometric Pressure. It will be noted in Fig. 34 that while the calculated curve is almost a straight line down to d = 0.5, below this point there is a decided bend to zero. The lower part of this curve was drawn from calculations. In order to check experimen- tally the above law over a wide range of 5, and also to show that the effect was the same whether the change was made by varying tem- perature or pressure, tests were made over a large pressure range. FIG. 35. Apparatus for determining the effect of pressure on strength of air A glass cylinder lined with tin foil 7.36 cm. in diameter with a small slit window in the center was used for this purpose. (-See Fig. 35.) Tests were made on wires 0.508 cm. to 0.157 cm. in diameter, and TABLE VIII. VARIATION OF STRENGTH OF AIR WITH PRESSURE Diameter of Brass Rod = 0.381 cm. in 7.36-cm. Diameter Glass Tube Covered with Tin Foil 60 ~ Pres. abs cm Hg Volts read (eff) Temp, cleg. C 5 sss 392Z 0v = ev g v max , measured kv /cm. ff v max , calculated f 0301 N 31s ( 1 + ^r) kv./cm r(log*R/r) kv./cm (eff ) 273 + t 5 3 2,880 27 0.069 5.08 7.19 7.80 10 7 4,580 24.0 0.141 8.09 11.45 12.40 11.2 4,920 27 146 8.68 12 28 12 15 19 3 7,400 27 252 13.06 18 47 18 58 27.7 9,550 27.0 0.362 16 87 23 85 24 06 36 6 12,000 27 0.478 21.20 30.00 29.60 46 4 14,450 25 0.612 25 50 36 07 35 70 47.0 14,600 27 0.614 25 80 36 50 35 80 55 7 16,300 27 0.728 28.80 40 75 40 75 60 17,760 25 5 0.792 31.35 44 30 43 50 66.0 18,400 27.0 0.867 32 50 46 00 46 75 75 21,100 25 997 37 25 52 70 52 25 56 DIELECTRIC PHENOMENA 55 50 g 45 |40 5 35 JO 3Q ^ 25 ^20 I 15 10 5 \ \ Wire RadxxisjB! .1905 ctm o a Experimental Values Drawn Curve -Calculated ^ ** ^ ^^ V s> 3^ -^ ^ ^ ^ ****^ ^ 4 ^ r^ <* S ^ / .2 .3 .4 .8 .9 1.0 373+* FIG. 37. Effect of pressure on the strength of , air. eu 55 Kfl \ ^ > Wire Eadius.127 cm. o Experimejatal Values Drawn, Carre - Calculated o ^> -^ B O 40 35 I 80 d 25 n 10 5 ^o ^ ^ ***** ^ ^ ^^ ^ \^ ^ ^ ^ A /<> / 4 / .1 .2 .3 .4 .5 a92B .6 .7 .8 .9 5 " 173+T 1,0 FIG, 38. Effect of pressure on the strength of air, VISUAL CORONA 57 a pressure range of 1.7 cm. to 76 cm. Table VIII is typical of observed and calculated values. Figs. 36, 37 and 38 show how these follow the previously predicted curve. A SA reduction of the values also confirms the above formulae. For concentric cylinders g v 316(1 -\ ^^) max. kv. per cm. \ Vor / For parallel wires g v = 305(1 -i 1 /=-) max. kv. per cm. The change in g v with the density is apparently due to change in the molecular spacing, and thus depends only upon the relative density and not the absolute density. Heavy CO 2 at the same pressure and temperature has the same strength as air. Corona in hydrogen, however, appears to start at a lower voltage than in air. Electric Strength of Air Films. If a definite amount of energy is necessary to start rupture at a finite distance a from the con- (P) L-a ( FIG. 39. ductor, with a surface gradient g v} it is interesting to speculate what will happen at very small spacings or when the distance between conductor surfaces is in the order of a. (See Fig. 39.) l As the free "energy storage," "accelerating" or "ionizing" distance is then limited, a greater force or gradient should be required when the distance between the conductors approaches a. Experiments were made to determine this, using spheres as elec- trodes. The ideal electrodes for this purpose would be concentric cylinders, but the use of these as well as parallel wires at small spacing seemed impracticable. Spark-over and corona curves were made on spheres ranging in diameter from 0.3 cm. to 50 cm. and spacings from 0.0025 cm. to 50 cm. This discussion applies only to spacings up to 2R where corona cannot form. 1 Actually, the "energy-zone" is not as shown, as the field is distorted at these small spacings. 58 DIELECTRIC PHENOMENA In these tests a 60-cycle sine wave voltage was used. For the small spacing the spheres were placed in a very rigid stand. One shank was threaded with a fine thread, the other was non-adjust- able (Fig. 40). In making a setting the adjustable shank was screwed in until the sphere surfaces just touched, as indicated by completing the circuit of an electric bell and single cell of a dry battery. A pointer at the end of the shank was then locked in place, after which the shank was screwed out any given number of turns or fraction of turns as indicated on the stationary dial. For larger spacings other stands were used. A typical spark-over spacing curve and corona spacing curve is shown in Fig. 41. Theoretically, up to a spacing of 2R corona cannot form but spark-over must be the first evidence of stress. Practically, corona cannot be detected at 60 until a spacing of SR is reached. This is because up to this point the difference FIG. 40. between the corona starting points and the spark point is very small. Above SR the spark-over curve approaches a straight line as in the case of the needle gap curve. The corona curve above 2R and the spark curve below 2R are apparently continuous. The gradient curve, Fig. 42, is calculated from the voltage curve, Fig. 41. Where the spacing is less than 0.54-\/J? the gradient increases first slowly and then very rapidly with decreasing spacing. Between X = 0.54^/R and 2R the gradient is very nearly con- stant. Above about 3.R spacing the gradient apparently increases. This apparent increase is probably due to the effect of the shanks, etc., which become greater as X is increased. The effect of the shanks is to better distribute the flux on the sphere surface, and cannot be taken account of in the equation for gradient. This was shown experimentally by using different sizes of shanks at VISUAL CORONA 59 the larger spacing. Thus, when the spacing is greater than 3R the sphere is not suitable for studying the strength of air, as the gradient cannot be conveniently calculated. It is hence not a suitable electrode for studying corona, as corona does not form until the spacing is greater than 2R. The maximum gradient at the surface of a sphere (non-grounded) may be calculated from the equation. 1 Spacing ~X~ Spacing -Jf- FIG. 41. Variation of corona and spark- FIG. 42. Variation of strength over voltages with spacing for spheres. of air with spacing for spheres. (13o) where X is the spacing E the voltage The gradient for the non-grounded case may be conveniently calculated by use of the table on page 27. The gradient on the line connecting the sphere centers at any distance a from the sphere surface may be calculated from the complicated equation 2 (X g* == 2X*[x*(f + 1) + 4(~ - a) V - 1)] [X \ 2 I 2 -4(f -a) (/-I)] _ (26) Some of the experimental values are given in Tables IX and X. Typical voltage gradient curves are shown in Figs. 43, 44 and 45. 1 G. R. Dean, G. E. Review, March, 1913. 2 G. R. Dean, also Physical Review, Dec., 1912, April, 1913. 60 DIELECTRIC PHENOMENA 8 J3 ' 2 ^ VISUAL CORONA 61 TABLE IX. SPARK-OVER OF SPHERES AT SMALL SP AGINGS Brass Spheres R = 3.33 cm , Diameter = 2-5/8 in. 60 ~ X Spacing * e eff s V2 (eeff ) ffmax. Kv 3 92fc = .' X X/R In. Cm, 273 +t S (corrected) kv./cm 001 00254 0.363 1.028 497 196 00076 002 0.00508 531 1.030 729 143 6 0.00152 003 0.00762 654 1.027 899 118 1 0.00228 004 0.01016 775 1 026 1 07 105 2 00305 005 0.0127 845 1 016 1.17 92 3 00382 010 0254 1 07 1.000 1.52 60 0.00764 020 0508 1 86 1 002 2.62 51 8 0.01528 040 1016 3 27 1 002 4.62 45 9 03056 075 1905 5 43 1 002 7 66 41 0.05730 100 0.254 6 92 1.002 9 77 39 5 0.0764 200 0.508 12 40 1.002 17 50 36.3 1528 0.300 0.762 17.70 1.002 25 00 35 4 2292 0.400 1.016 22 70 1.002 32 00 34 8 3056 500 1.270 27.75 1 002 39 20 34 9 0.382 TABLE X. SPARK-OVER OP SPHERES AT SMALL SPACINGS Brass Spheres R = 12.5 cm , Diameter = 9 84 in 60 ~ X Spacing Kv. (read) s 3926 vs Qm a*. X/R In. Cm. ~273+f 5 (corrected 1 * ~~ X f kv./cm 005 0.0127 0.807 1 023 1 116 87.9 0.00101 010 0.0254 1.220 1 021 1.689 66.5 0.00203 020 0.0508 2 050 1 031 2 849 55 9 0.00406 040 1016 3 38 1 022 4.68 46 2 0.00813 100 0.254 7 03 1.020 9 75 38.6 0.0203 200 0.508 12 54 1,012 17 44 34 8 0.0406 300 762 17.91 1 016 24 92 33.5 0.0609 400 1 016 22.82 1.010 31.76 32 0.0812 500 1 27 27.63 1.010 38 67 31 5 0.1016 1 000 2 54 53 1.000 . 74.90 31 6 0,2032 1 500 3.81 75.3 1.000 106.30 30.9 3048 2 000 5.08 96 4 1.000 136.20 30.5 0.4064 2 500 6 35 117.4 1.000 166.00 30 7 0.5080 3 000 7.62 139.2 1.000 196'. 90 31.2 0.6096 3.500 8.89 158.0 1.000 223.40 31 3 0.7112 4 000 10 16 174.9 1.000 247 10 31.0 0.8128 4 500 11 43 190.8 1.000 269 50 31 0.9144 5.000 12 70 203 6 1.000 287 20 30.8 1.0160 *At low air density and small spacings correction must be made by Paschen's Law. See page 196. Also appendix. 62 DIELECTRIC PHENOMENA In Table XI are tabulated, for different sizes of spheres, the spark-over gradient at the constant part of the curve, the aver- age gradient between X = 0.54^/R and X = 3R, and the approxi- mate minimum spacing at which the gradient begins to increase TABLE XI. MAXIMUM RUPTURING GRADIENTS FOR SPHERES (Average for Constant Part of the Curve) R Radius m crn Spacing X, where g a begins to increase (cm ) ff s max kv./cm for constant part of curve 159 18 63 8 238 25 55.6 356 0.26 51 4 0.555 0*40 46 9 1.270 51 40.0 2 540 85 36 8 3.120 35.8 3.330 95 34 8 6.25 1 30 32 5 12 50 2 31.3 25.00 30 > 60 a 55 S 50 0.45 f # 35 | S 25 ! 2 215 % 5 I \ \ V r^ . ~o -* 91234567 89 10 11 121T Radius in cme* FIG. 46. Variation of the apparent strength of air with sphere radius Points measured gradient from- constant part of curve. Drawn curve, calculated from equation (27). in value. The gradient-radius curve is plotted in Fig. 46. This curve is very closely given by the equation ff* (27) VISUAL CORONA 63 which has exactly the same form as the similar curve for cylinders. The value of g is, however, lower than for the balanced field of a "dre in a cylinder. % 'or a wire in a cylinder g = 31 'or parallel wires 'or spheres go = 30 , Vr / 27.2 g v + 0.54 \ VB) (25a) (256) (28) It is probable that the true strength of air is 3 1 kv. per centimeter 3 represented by the balanced field, it is apparently less for parallel ires due to the unbalanced field, and still less for spheres where ie field is unbalanced to a O reater extent. The curve between the sphere radius and the ap- proximate minimum spacing below which the gradient be- gins to increase appreciably is plotted in Fig. 47 from Table XI. The curve is rep- U 1 d % OO < O * All J.4. Radius in Centimeters > between Spheres j r . M r r r 5 to # o> oo o ^ ^ ^ ^ ^ -"'' S J S S 1-8 1 i ft ft * / / f FIG. 47. Sphere spacing "below which apparent strength begins to increase. resented by the equation X = Q.54VR (29) which means that when the spacing is less than 0.54A/B the gradient increases in value, at first slowly, then very rapidly. It is now interesting to investigate the meaning of equation (27). In Fig. 48 the exact gradient is plotted from equation (26) for different distances from the sphere surface on the line con- necting the centers and at given spacings as indicated by the small diagram in the upper corner of the figure. It is seen that for small distances from the sphere surface the curves for the differ- ent spacings fall together. Over the small range the gradient g a at any point a centimeters from the sphere surface on the center line may be found approximately from (R + M)\X) J (30) The only reason for giving this approximation, which holds only for very small values of a and is only true when a = 0, is 64 DIELECTRIC PHENOMENA that (26) is too complicated to handle. The error due to this approximation is shown in Table XII. TABLE XII R - 1 27 cm Energy distance, a = 27 \/K "= 3 cm R - 12 5 cm. Energy distance, a = 95 cm a 0a> Exact A 0, Approx X a ffa, Exact Approx X 0.0 39 9 39 9 76 31 3 31 3 4 1 34 6 34 76 2 30 3 30 3 4 2 31 9 30 76 4 29 5 29 4 4 4 29 7 24 1 76 6 28 6 28 5 4 8 28 3 27.7 4 0.0 39.9 39 9 1 21 1 27 5 26 9 4 0.1 34 2 33 4 1 21 2 30 5 29 5 1 21 31 3 31 3 10 4 26 5 23 7 1 21 2 30 3 30 3 10 4 29 5 29 4 10 6 28 6 28 7 10 8 28 27 7 10 1 27 5 26.9 10 Then ff* = E*(R_ f \ R\X f ) mathematical. = oll4- -^~\ experimental for approximately y* y ( -r ^/gy constant part of curve, 77T / T~) v ^ p " . (^/ ) approximate mathematical. (Jti -(- j&a) \3L / Equating (I3a) and (27) E. (13a) (30) which is the same form as (30) and means that at a distance cm. from the sphere surface the gradient at rupture is always approxi- mately constant and is g .__ As breakdown must take place at approximately a = 0.27 V^B cm. from the sphere surface, the VISUAL CORONA 65 gradient should begin to increase at the spacing 2a = 0.54 \/R. This is approximately so as shown in Fig. 47 and equation (30). The increase is at first slow at X = 2a, and very rapid at X = a, Fig. 48 shows that at a = Q.27\/R the gradient is not exactly constant for different spaeings, or the curves do not fall together. 3b .34 32 Iso. i: 3 24 S22 W iis lie 5l2 10 3alc ulatioj^ of ( Gra|die: it ^ j bet wee aS] !>hei es V ^ ; N ^5 i :m, 5 3 ^ 5C 2 c en O - -4t- 34AU ^ K -^ 7 1- 2lL5 y ^5 *-*. - = 4 cm, ffd ss. Gradient on Line AJ3 at Distance a from Surf ace of Si 12.5 cm. Spheres ^^^ 5vv )here s; ^ ^> ^ ^ >v, ^ a: =10 cm <^ ^-. ""*-- ^ "***^ -^ ^. "~-^ L5 cm. T*J XLo c m. = N CO 00 OJ -* X 100 200 300 400 500 600 700 800 900 1000 Frequency Cycles/Sec, FIG. 49. Variation of the apparent strength of air with frequency. of frequency on g v for the practical range of 25 to 60 cycles, if any, is very small and can be neglected. A few measurements are shown in Fig. 49. For the test range it is difficult to tell whether the slight variations are due to changes in wave shape or to fre- 66 DIELECTRIC PHENOMENA quency. There is a possibility of frequency entering this as a function: Investigations up to 1000 cycles show very little if any change. In this investigation the sine wave voltage was measured with a static voltmeter calibrated at 60 cycles. Measurement at 30,000 cycles (sine wave from a generator) made by the static volt- meter showed a slightly lower voltage than at 60 cycles. 1 Direct current points by Watson are given in Fig. 49. See appendix. Over the commercial range of frequency, however, there is no appreciable effect of frequency. For transient corona see page 108 and appendix. Effect of Oil, Water orDirt on the Visual Corona Point These tests were made in a manner exactly similar to the dry tests. 10 20 30 40 50 Spacing m eras Between < 10 20 30 40 50 60 70 Spacing In cms Between Centers FIGS 50 and 51. Spark-over and corona voltages for parallel wires. (Wire surfaces dry, wet, and oiled. Max. kv to neutral, s = 1. Fig. 50 Wire radius . 205 cm. Fig. 51. Wire radius 129 cm.) In the oil tests, the surface of the wire was coated with a thin, even film by means of an oiled cloth. For the wet tests water was sprayed on the conductor surface before each reading by means of an atomizer. Figs. 50 and 51 are dry, wet and oil curves for two different sizes of wire. For spark-over, both water and oil have approximately the same effect, that is, give very nearly the same spark-over voltage for all sizes of conductor. The curves very closely follow the needle gap curve. For corona, water very greatly lowers g v . Oil lowers g v but to a See pages 106, 107, VISUAL CORONA 67 much less extent than water. When the conductor is very small the per cent, increase in diameter due to oil more than com- pensates for the lowering effect. The approximate apparent visual corona gradient for oil and water coated conductors may be found Water surfaces by fine spray or fog _ J- , 0.815 \ . g v = 9( 1 H -- 7=- ) max. kv. per cm. \ V r / Oil film surfaces g v = 19( 1 +' V ) max. kv. \ Vr/ per cm. See Fig. 52. If a water coated wire above the visual corona point is exam- ined in the dark, it has the appearance of an illuminated atomizer. The surface quickly becomes dry. 50 240 p30 W20 FIQ. 52. Apparent strength of air around wires with wet and oiled surfaces. Dirt on the surface of the conductor, by increasing the gradient, causes local brush discharges, and if the surface is rough, corona starts at a lower voltage. This is taken care of in the formulae by an irregularity factor m v . Thus for a weathered or oxidized wire 0301X VTr/ g v = g m v d( 1 The corona starting voltage for wet or oiled wires may be found by calculating g,/in the above equations and substituting in equation (20). DIELECTRIC PHENOMENA Conductor Material. With the same surface condition the visual corona point is independent of the material. This is shown in Table II. Humidity. Tests made over a very wide humidity range show that humidity has no appreciable affect upon the starting point of visual corona. After corona is present humidity has an effect on the spark-over voltage. This is discussed in Chapter IV. lonization. Change of initial ionization of the air even to a considerable extent has no appreciable effect on the starting point of corona. This was found by test by increasing the voltage on the wire in the cylinder until considerably above the corona voltage, and then, while the cylinder was full of ionized air, lower- ing the voltage below the corona point and again raising it until glow appeared. The starting point was not appreciably changed. Initial ionization should, however, effect the time in which the discharge takes place. This will be discussed later. Current in Wire. A test was made to see if heavy currents flowing in the wire would change the starting point of visual corona. The test arrangement was as shown in the Fig. 53. FIG. 53. Apparatus for measuring corona starting point with current in the wires. Tests were made with both a.c. in phase and out of phase, and d.c. in the wire. The results are given in Tables XIII, XIV and XV. The temperature of the wire was measured by the resist- ance method. The values in the last column are all corrected from the wire temperature to 5 = 1. If the current has no appreciable effect, as appears to be the case, these should all be equal. The variation is probably due to difficulty in getting the VISUAL CORONA 69 TABLE XIII. CORONA STARTING POINT WITH CURRENT FLOWING THROUGH WIRE Concentric Cylinders Radius of wire 129 cm. Radius of cylinder . . . 5 46 cm. Kv. eff. Amp d c. Average temperature Barom cm 6 (using wire temp ) ffv g v reduced to 51 Air Wire 20 26 26 75 6 991 58 4 58.9 19.7 15 2 26 32 970 57 5 59 2 19 4 31 4 26 48 922 56 7 61.4 18.5 39 26 64 878 54 1 61 6 17.8 49 2 26 82 824 52 63 1 16 9 75 26 120 0.753 49 4 65 6 20.4 23 23" . . . 1 000 59 6 59.6 20.3 18 23 27 987 59 3 59.9 19.4 33 23 50 917 56 7 61 8 17 9 50 8 24 91 813 52 2 64 2 12.9 99.6 24 320 500 37 6 75 2 16.4 67.6 26 102 790 47 9 60.6 13 9 78 6 26 212 610 40 8 67 16 1 61 6 26 144 710 47 66 2 TABLE XIV. CORONA STARTING POINT WITH CURRENT FLOWING THROUGH WIRE Concentric Cylinders Radius of wire . . 205 cm- Radius of cylinder . . 5 46 cm. Kv. eff. Amp Average temperature Barom cm 5 (using wire temp ) ff* g v reduced to S = 1 Air Wire 25.3 14 (d.c.) 23 23 76.2 1 '01 f 53 15 52 6 25.2 23 23 76 2 1.01 53 52 5 25.2 14 (a.c. 23 23 75.8 1 005 52 8 52 6 in phase) 25.1 14 (a c. 23 23 75.8 1 005 52 6 52 3 out of phase) 25.1 23 23 75.8 1.005 52 6 52.3 25.2 24 24 75.25 0.994 52 8 53 2 25 2 14 (d.c.) 24 30 75.25 974 52 8 54 3 25.2 34 (d c.) 25 60 75.25 886 52 4 59 1 23.8 56 (d.c.) 29 60 75.25 886 50 56 3 23 3 70 (d c.) 30 73 75.25 853 48 8 57 3 21 8 114 (d c.) 110 75 25 771 45 7 59 2 25.0 60 (d c.) 31 31 75 25 971 52 4 53 9 25.0 31 31 75 25 971 52 4 53 9 24.8 23 (a.c.) 31 44 75.25 0.931 52 55 8 70 DIELECTRIC PHENOMENA TABLE XV. CORONA STARTING POINT WITH CURRENT FLOWING THROUGH WIRE Concentric Cylinders Radius of wire Radius of cylinder 0.476 cm. 5.465 cm. Average Kv eff Amp d c temperature Barom cm 5 (using Q-o g v reduced Q ft .5 ]^ Air Wire 36.5 27 27 75 5 985 44 3 45 36.5 80 27 27 75.5 0.985 44.3 45 'exact temperature of the air. The air immediately surrounding the wire is assumed to be at the same temperature as the wire. This causes a correction that is too large. Current flowing in a wire thus probably does not appreciably effect the corona point unless the temperature of the wire is increased. Stranded Conductors or Cables. While the visual critical corona point is quite sharp and definite for wires, it is not so for .8 1.0 Diameter in cms. FIG. 54. Apparent visual critical corona voltages for parallel cables. Numerals denote number of strands: I, polished copper wire; II, decided corona on cable, o; III, local corona all along cable, x. cables or standard conductors. Corona, after it first appears, increases gradually for a considerable range of voltage until a certain definite voltage is reached where the increase is very rapid. The first point has been called the local corona point, and the second point the decided corona point. The curve, Fig. 54, for these corona points is compared with the curve for a smooth VISUAL CORONA 71 g* = g mJ 1 + conductor. The starting point for cables may be found by the use of an irregularity factor, m*. 0.301 \ . 7=- I kv. per cm. V r I where m v = .82 for decided corona m v = .72 for local corona r = overall radius of cable. This applies to cables of six strands or over. It is interesting to note that for the decided corona point the visual critical voltage of a cable is about 3 per cent, lower than that of a wire with the same cross-section, or, more exactly "the diameter of a solid wire with the same critical voltage is about 97 per cent, that of the wire having the same cross-section as the cable." 1 This is shown in Table XVI. TABLE XVI. EFFECT OF STRANDING Whitehead, AJ.E.E, June, 1911, Table III Cables, Diameter Diameter solid Diameter solid Pitch of spiral strands outer over all of equal section of equal crit- ical volts C/B C/A layer U) (B) (C) Cm. Diameters 3 349 272 247 907 0.708 3.81 10 9 4 0.404 332 320 965 0.792 3 49 8 6 5 45 0.381 0.370 0.971 822 4.44 9 9 6 49 0.430 420 0.975 0.857 6 02 12.3 7 0.541 0.480 0.465 969 868 6.66 12.3 8 589 0.530 0.516 0.975 877 6.35 10 8 9 64 0.581 0.567 0.977 886 6.98 10.9 3 336 27 0.307 0.767 616 None None 4 378 312 25 0.802 665 None None Conductors of the Same Potential Close Together. When conductors of the same potential are arranged close together the critical breakdown voltage is much greater than that of a single conductor or when they are far apart. The simplest case, that of two, is shown in Fig. 55. The two conductors for a given test were kept at a constant distance S/2 from the ground plate. Potential was applied between the conductors and plate. The separation m was then varied and critical voltages read at differ- 1 Whitehead, Dielectric Strength of Air, AJ.E.E , June, 1911. 72 DIELECTRIC PHENOMENA ent spacings. Refer to Fig. 56 (0. 163-cm. wire 30 cm. from neutral plane). When m = 0, e v = 31.5 eff. As the spacing m was in- creased, e v increased to a maximum of 35.8 kv. With increasing m } e v then gradually decreases to a constant value which is the same as that for a single wire. The maximum voltage is about 5 Ht t* ^40 S3 5, i > 30! Ground Plate gle Wire 5 10 15 20 25 30 35 40 45 50 Separation -m - fttn. FIG. 56. Critical voltage on two conductors at same potential, and conductors at the same potential and various separations (see Fig. 55). FIG. 55. Arrangement for two ondu plate. per cent, greater than the critical voltage of a single conductor of the same cross section. With the same amount of conductor material, much higher voltages can be used without corona loss when the conductor is pnrninnn 510152025303540455055 Spacing -s-cm. FIG. 57. Conductors of the FIG. 58. Critical voltages for conductors same potential arranged in a arranged as in Fig, 57. triangle. split up into three or more small conductors, properly arranged, than with a single conductor. The results of tests made on a single-phase line with split conductors arranged in a triangle as in Fig. 57 are 'given in Fig. 58. Fig. 58 shows curves for a single split wire and also for a single wire of a cross section equal VISUAL CORONA 73 to that of the three split conductors. Fig. 59 shows how the voltage varies with varying m. With the split conductor arrangement, in the special case given, the critical voltage is from 20 to 30 per cent, greater than that of a single wire containing the same amount of material. Whitehead has made similar tests on three wires in a triangle and also four wires placed on a square in the center of a cylinder. Critical Yoltage-0 v - KV 8 3 8 8 & N \ N, Equivalent Wire 8 ugle 1 Vire ( 101520253035404550 Separation W, Cm FIG. 59. Critical voltage of conductors arranged as in Fig. 57. (S = constant = 40 cm., m varying.) He finds 16 per cent, increase for three wires and 20 per cent, for four over the critical voltage of a single conductor of the same total material. STHOBOSCOPIC AND PHOTOGRAPHIC STUDY Photographic Study. A photographic study of corona on wires and cables was made as follows: Two parallel conductors were spaced 122 cm. between centers. The camera was focused on one conductor only. The distance to the lens was such as to show the conductors at approximately actual size. An exposure was made for a given time at a given voltage. The plate wsis then shifted slightly, the voltage increased and a second exposure was made for the same time. That is, a given series shows the same part of the same single wire at different voltages. This operation was repeated until the series for a given wire was complete. A glass lens was used unless otherwise stated. (See Fig. 60.) These photographs are shown in Figs. 61 to 68. Photographs 67 and 68 were made to show the effects of mois- ture. In Fig. 67 the stranded cable was brought up to the critical point. Water was then thrown on the cable. The result is shown in Fig. 68. What was a glow at the surface of the dry 74 DIELECTRIC PHENOMENA cable became at the wet spots, a discharge extending from 5 to 8 cm. from the conductor surface. The discharge has the appear- ance of an illuminated atomizer. Diameter of Corona. On a smooth wire the boundary line of corona appears to be fairly definite. The apparent visual diame- ter may be measured by viewing through a slit. The apparent diameter may also be found photographically. If the photo- graph is made through a quartz lens the ultraviolet rays will not be cut off from the plates as when a glass lens is used. { Whitehead has made some measurements on the apparent diame- ter, comparing the visual method and the photographic method with both quartz and glass lenses. He finds that the apparent diameters are respectively by the visual, glass lens, and quartz lens methods in the ratios of 1 : 1.6 : 1*9. l It therefore appears that there is a considerable content of the corona at the ultra- violet which is not visible to the eye. As soon as corona appears it seems to have a definite finite thickness. Conductors - Direction of Shift * ' 4 FIG. 60. Method of making corona photographs. T^ABLE ' XVJI. DlAMETEB OF CoBONA QN WlBE IN THE CENTER OF A CYLINDER Diameter wire 0.233 cm,, 18.6-cm. cylinder Fig. 9 (Wnitehead, A.LEE., June, 1912) : JKiIovolt9 Diameter* corona, mm Time, min. Lens No Diameter corona, visual method, ' , mm. 22.5 5,5 2 Glass (a) * ' 27.5 9.3 2 Glass (b) 32.5 11 1 2 Glass (c) 6.7 1 Whitehead, Electric Strength of Air, A.I.E.E., June, 1912. JP IG m Corona on bright tinned ' - :; - - 0-051 cm;' wire. Diameter, " FIG 62 Corona on copper wire polished after each exposure. Diameter, 0.186 cm. (Facing page 74.) FIG. 63. Corona on a polished copper wire. Diameter ,0.1 86 cm. Oper- ated at 200 kv., then allowed to stand idle. (This shows effect of oxidation.) FIG. 64. Corona on a weathered galvanized iron wire. Diameter, 168 cm. FIG. 65. Corona on a 1.25 cm. polished brass rod and unpolished copper cable. FIG. 66. -Corona on a No. 3/0 weathered cable. (Following Fig. 64.) FIG. 67. Corona on a No. 3/0 line cable. Dry. FIG. 68. Corona on a No. 3/0 line cable. Wet. (Facing page 75.) VISUAL CORONA 75 TABLE XVIII. DIAMETER OF CORONA, WITH AND WITHOUT ULTRAVIOLET CONTENT (On a Wire in the Center of a Cylinder) Exposure 20 min., 32.5-kv. cylinder, diam. = 186 cm. (Whitehead, A I.E.E., June, 1912) 232-cm wire 316-cm. wire 399-cm wire Quartz and glass Quartz alone Quartz and glass Quartz alone Quartz and glass Quartz alone 12 12 4 12 5 13 3 11 4 13.0 11 5 12 6 13 14 11.6 13.0 11 5 12 6 13 14 12.0 12 8 11 4 13 12 8. 14 12 12 8 11 6 12 6 12 8 13 8 11 7 12.9 Figs. 69, 70 and 71 and Tables XVII and XVIII taken from Whitehead are self explanatory. Fig. 72 1 shows the apparent diameter of corona on a given wire. At the start the corona 1.4 s -1.2 i LO 60.8 |o.e i 0.4 ^0.2 Diameter of Corona cm. p p p p f* f M tO rt^ 0> CO K> (*x ^ X s < X"^ ^ x^ / s~ y D iame ter o f Wi e .233 cm. 20 22 24 26 28 30 32 34 36 Kilo- Volts Effective 20 22 24 26 28 30 32 34 Kilo-Vlf& Effective FIG. 72. FIG. 73. Figs. 72 and 73. Diameter of corona (0.233 cm. wire in 18.6 cm. cylinder). appears to take immediately a definite finite thickness; the rate of increase is then quite rapid, but gradually assumes a linear relation. 1 In Fig. 73 is a curve through the same points. Throughout this curve the correction of 1.18 has been used to include the ultraviolet. How- ever, near the starting voltage the corona seems to be very largely ultraviolet. This explains the low point at 22.5 kv. 76 DIELECTRIC PHENOMENA A study of the power loss equation leads one to suspect that the mechanism of corona loss is more complicated than might at first be supposed. This is also indicated by many peculiar phenomena of the spark discharge. For instance, while investigating a.c. spark-over and corona for parallel wires it was observed that when the end shields were not used, and the wires came directly in contact with the wooden wheel supports, corona often appeared to bridge completely between the conductors without a dynamic arc. In this case it seemed possible that the corona on the posi- tive wire extended out farther than the corona on the negative wire and that the positive discharges overlapped and combine in the eye, giving the effect of a single discharge completely across between the conductors. In the hope of throwing further light on the discharge and loss mechanism, an investigation of corona and spark was made with the help of the stroboscope. A needle gap was first arranged across the transformer with a high steadying resistance. The impressed voltage was adjusted until corona appeared all the way between the conductors as in Fig. 74. Examination of this was then made through the stroboscope which was so set that the right needle, Fig. 74(2), was seen when positive, and the left when negative. To the eye, the discharge from the positive needle has a bluish- white color and extends out a considerable distance, the negative appears as a red and hot point. This arrangement may, therefore, be used as a rectifier. The photograph shows more of the negative than is seen by the eye. Fig. 74(1) is the discharge as it appears without strobo- scope, 74(2) with the right needle as positive, 74(3) with strobo- scope shifted 180 deg. to show left needle as positive. In 74(4) the stroboscope has the same position as 74(3), but the voltage is higher, and many fine " static" sparks can be seen. If voltage above the visual corona point is impressed on two parallel polished wires a more or less even glow appears around the wires. After a time the wires have a beaded appearance. On closer examination the beads appear as reddish tufts, while in between them appears a fine bluish- white needle-like fringe. On examination through the stroboscope it can be seen that the more or less evenly spaced beads are on the negative wire, while the positive wire has the appearance, if not roughened by points, of a smooth bluish- white glow. At " points" the positive discharge extends out at a great distance in the form of needles; it is possible that it always extends out but is not always visible except as sur- DIAMETER OF CORONA. FIG. 69 (Upper). Diameter of corona on 0.233 cm. wire in 18.6 cm. cylinder. e v =21.5 kv. Glass lens kilovolts 22.5, 25, 27.5, 30, 32.5 respectively. (Whitehead.) FIG. 70 '(Middle). Diameter of corona showing effect of ultra-violet, (a), 0.232 cm. (6), 0.316 cm. (c), 0.399 cm. Left side of (a)(6)(c), quartz lens. Right side of (a) (6) (c), glass lens. (Whitehead.) FIG. 71 (Lower). Corona on 0.233 cm. wire, at 22.5, 27.5, 32.5 kv. e v = 20.75 kv. Glass lens. (Whitehead.) (.Facing page 76.) 6^ e f'% %' 1 (1) Without stroboscope, 72,000 volts. Left(-) (2) With stroboscope, 72,000 volts. Right (+) Left (+) (3) Same as (2), stroboscope rotated 180. Right (-) Left (+) (4) Same as (3), voltage increased to 84,000. Right (-) FIG. 74. Corona between copper needle points. 20.5 cm. gap. (1) Without stroboscope. (+) (2) With stroboscope. Right (-) Left (-) (3) With stroboscope Right (+) (3) With stroboscope rotated 180. FIG. 77. Corona on parallel wires.- No. 13 B. and 8. copper wire. Spacing, 12 . 7 cm. Volts, 82,000. Left (-)" Right (+) FIG. 79. Polished brass rod. Diameter. 475 cm. Spacing, 120 cm., Volts, 150,000. Note that negative "beads" are just starting to form. FIG. 78. Section of wire (Fig. 77). /< Dead." Bright spots position of negative "beads." Left(-) Right ( + ) FIG. 80. Copper wire. Diameter 0. 26 cm. Spac- ing, 120 cm. Volts, 200,000. Polished at start. Note negative corona apparently following spiral (Following Fig. 77.) ' l grain" of wire. VISUAL CORONA 77 face glow. Thus, the appearance of beads and fringe to the un- aided eye is really a combination of positive and negative corona. In Figs. 75 and 76 two wires are placed close together at the top. The bottom is bent out and needles are fastened on. Fig. 75 is without a stroboscope. Fig. 76 is taken with a stroboscope set to show positive right and negative left. Thus, positive and nega- tive coronas for points and wires are directly compared. Fig. 77(1) is taken without the stroboscope, (2) with right negative, (3) with stroboscope shifted 180 electrical degrees to show the right positive. These wires were, at the start, highly polished. At first corona appeared quite uniform, but, after a time, under voltage, the reddish negative tufts separated, more or less evenly spaced as shown. 24(2) is the same with stroboscope shifted 180 deg. Fig. 78 shows a section without voltage. The bright spots are still polished and correspond in position to the negative tufts. The space in between is oxidized. Thus, the negative discharge appears to throw metal or oxide from the surface at discharge points. This takes place with either copper or iron wire. Fig. 79 shows positive and negative corona on wires widely spaced to get uniform field distribution. A close examination of the negative shows beads about to form. Fig. 80 shows a similar pair of conductors. The negative in this case has formed a spiral, apparently following the grain twist of the conductor. A large fan-like bluish discharge is often observed extending several inches from the ends of transformer bushings, points on wires, etc. This discharge has the appearance of a bluish spray, reddish at the point. The stroboscope shows that the bluish spray is positive, while the red point at the base of the spray is negative. Fig. 81 shows one of two parallel polished rods (120 cm. spacing), supported at the top and brought to sharp points at the bottom; 81(1) shows how each wire appears without stroboscope; 81(2) is the wire when positive, 81(3) the wire when negative. Note the dark space on 81(3) between the point and negative corona spiral of tufts. 81(1) shows this space to have only the positive glow. Water was placed on a pair of parallel conductors. At the wet places the positive corona extended out in long fine bluish-white streamers. (See Fig. 82 without stroboscope.) With certain forms of dirt on the wires the negative corona appears as red spots, the positive always as streamers. It is also interesting to note that if a uniformly rough wire is taken, as a galvanized wire or 78 DIELECTRIC PHENOMENA u weathered" wire, the positive appears as bluish needles, while the reddish negative is more uniform than on the " corona-spotted " polished wire, in which case the negative corona appears as con- centrated at the non-oxidized spots. It is probable that the polished spots are kept so by metal and oxide being " thrown out" at the negative, as suggested above. Mechanical Vibration of Conductors and Other Phenomena. Several years ago a pair of 20 mil steel conductors, 500 ft. long, were strung at about 10-ft. spacing, for power loss measurements. It was noticed at high voltage that the conductors vibrated, starting with a hardly perceptible movement, which in a few minutes had an amplitude of several feet at the center of the span. Generally one wire vibrated as fundamental, the other as third harmonic. The period of the fundamental in this case was about one per second. Figs, 83 and 84 show this condition repeated in the laboratory on short lengths of conductor. In Fig. 83 one wire is vibrating as the fundamental, the other as the second harmonic. The motion is rotary. For the wire with a node in the center, Fig. 83, it is extremely interesting to note that for about one-half of the ro- tation the wire appears very bright, for the other half rota- tion the wire is much less bright. This seems to mean that each part of the wire is rotating at the power supply frequency 60 cycles per second. Hence, it has the effect of the stroboscope, and for part of the rotation there is always negative corona and for the other part always positive corona. Oscillograms of Corona Current. Bennett has made some very interesting oscillograms of corona current. 1 Fig. 85 (a), (&) and (c) shows the voltage wave applied between a cylinder and a concen- tric wire, and the resulting current. The part of the wave above the zero line occurs when the wire is , and that below when the wire is +; (a) is for a voltage very slightly above the critical voltage and shows a very sudden sharp hump in the current wave when the wire is +, and a spread out hump when the wire is . This gives the appearance of corona starting at a slightly lower voltage on the + wire; (b) and (c) show the positive and nega- tive humps at highe!r voltage. The oscillation is caused by the sudden " corona spark" discharging through the reactance and capacity of the circuit. Some tests made on the starting time appear to show that sev- eral cycles are necessary for stable conditions. 1 Bennett, An Oscillographic Study of Corona, A.I.E.E., June, 1915. FIG. 83. Mechanical vibration of parallel wires due to corona. FIG. 84* Mechanical vibration of parallel wires due to corona. (Facing page 7&) FIG. 85. Oscilligrams of corona current. (Bennet, A. I. E. E. 7 June, 1913.) CHAPTER IV SPARK-OVER By spark-over is generally meant a disruption of the dielectric from one conductor to another conductor. Corona is the same phenomena spark from a conductor to space or Jocal spark-over. Parallel Wires. If impressed voltage is gradually increased on two parallel wires placed a considerable distance apart in air, so that the ratio S/r is above a certain critical value, the first evidence of stress in the air is visual corona. If the voltage is still further increased the wires become brighter and the corona has the appearance of extending farther out from the surface. Finally, when the voltage has been sufficiently in- creased, at some chance place a spark will bridge between the conductors. When the spacing is small, so that S/r has a critical ratio, spark and corona may occur simultaneously, or the spark may bridge across before corona appears. If the spacing is still further reduced so that S/r is below the critical ratio the first evidence of stress is complete spark-over and corona never appears. (See page 27.) Extensive tests have been made. 1 The method of making tests was to start at the smaller spacings with a given yalue of r and measure the spark-over voltage. Unless otherwise stated the frequency used was 60 ~. When the spacings were above the critical ratio of S/r, and corona formed before spark-over, the corona voltage was noted first. The voltage was then increased until spark-over occurred. The spark-over point is not as con- stant or consistent as the corona point and is susceptible to change with the slightest dirt spot on the conductor surface, and any unsteady condition in the circuit, humidity, etc. At the beginning of the tests it was found necessary, in order to get consistent results, to put water tube resistances in series with the conductors to eliminate resonance phenomena. These resistances were High, but not sufficiently so to cause an appreciable drop in voltage before arc-over. Table XIX is a typical data table. Each point is the average of a number of readings. 1 See Law of Corona II, AJ E.E., June, 1912 79 80 DIELECTRIC PHENOMENA TABLE XIX. CORONA AND SPARK-OVER FOR PARALLEL WIRES , Temperature 17 deg C , bar 75.3 cm. Wire No 0, diameter 825 cm. Test No. 166 values read 60 ~ No wire, corrected to 25 C , 76 bar. Spacing Effective kv. to neutral Maximum values to neutral Maximum Cm S Corona e Spark e a Corona e v Spark e a Corona g* Spark g a 2 54 None 15 8 21 9 41 4 3 81 None 22 5 31 2 42 5 5 08 None 27.3 37 9 . 43 2 6 35 None 31.05. 43 2 43 8 7 62 None 35.0 48 5 . 44 9 8 89 None 37 35 51 8 45 10 16 40 4 40 9 56 56 7 44 44 6 12 70 41 8 42 1 58 58 1 44 44 1 13 97 43 7 46 60 7 60 5 44 2 46 7 15.24 45 9 48 1 63 6 67 45 1 48 9 15 78 46 6 54 1 64 8 75 43 8 50 8 20.32 48 9 59 6 67 7 82 8 44 53 7 22 86 50 1 66 2 69 7 91 7 43 7 56 8 25.40 51.1 71 5 70 7 99 2 43 1 ,60 4 27.94 52 1 79 72 4 109 7 42 9 65 1 30.48 53 1 84 5 74 117 42 9 67 9 33.02 54 1 89 6 74 8 124 42 4 70 2 35.56 55 1 95 5 76 5 132 5 42,6 73 9 38.10 56.1 102 3 77 8 141 9 42 7 77 8 40.64 57.1 106 5 79 4 149.0 42 9 80 5 60.96 63.3 87 42 9 . In columns 4 and 5 are voltages reduced to the maximum value to neutral and corrected to standard 5. Column 6 gives the surface gradient for corona. Column 7 gives the surface gradient for spark, up to the spacing where corona starts first; above this critical spacing it gives the apparent surface gradient as the conductor above this point must be larger on account of corona. As the field around the conductors at the small spacings is very much distorted it is necessary to use formula 12(a) or 12(&) to calculate the surface gradient. Fig. 86 is a typical curve. Voltage is plotted with spacing for spark and corona. Up to spacing 12.4 cm. there is spark-over before corona. This curve seems to be continuous with the corona curve which starts at this point. The spark curve here SPARK-OVER 81 branches and is very close to a straight line within the voltage range. In Fig. 87, the surface gradient curves are plotted. The 53 2 ! i 15U 7140 |130 ~ri2o guo gioo > M 80 ^ 70 5 60 1 50 |40 a so 5 20 10 if f i ** S ff ore M> ^5 ' f ^ ^, x* 10 20 30 40 50 60 70 Spacing in cm between Wire Centers 10 20 30 40 50 60 TQt Spacing in cm between Wire Centers FIG. 86. Spark-over and visual FIG. 87. Corona gradient and ap- corona voltages. parent spark gradient. (Parallel polished copper wires, 0.825 cm. diameter. 8 = 1.) corona gradient is a straight line parallel to the X axis with a slight hump at the critical ratio of S/r. The apparent spark 10 25 30 15 20 Spacing mem. FIG. 88. Apparent spark-over gradients for parallel wires. (Points meas- ured, curves calculated.) gradient is also a straight line, within the test range. It inter- sects the corona line at the critical ratio point, or at what may be 82 DIELECTRIC PHENOMENA termed the triangular point, and extended it cuts the g axis at g = 30. These are characteristic curves. (See also Figs. 50 and 51.) For a given spacing the spark-over voltage increases as the size of the conductor decreases. It is important to note that for all sizes of wire the spark gradi- ent curve extended as a straight line cuts the gradient axis at approximately g = 30. Spark curves extended as straight lines through the critical ratio point and intersecting the gradient axis at g = 30 are shown in Fig. 88. The triangular point or critical ratio of S/r is tabulated in Table XX. Its average value is TABLE XX. CRITICAL RATIOS S/r EXPERIMENTAL VALUES Intersection point of g v and g, Size, B &S Radius cond , cm 5, cm S/r Size, B &S Radius cond , cm S, cm S/r 461 13 5 29 3 6 205 6 2 30 2 412 11 7 28 4 8 -0 162 4 8 29 6 2 327 10 2 31 2 10 129 4 31 4 260 7 9 30 4 12 103 3 29 1 5 230 7.3 31 7 Average 30 1 S/r = 30. If it is assumed that the spark-gradient curve is a straight line the conditions are, that it must cut the corona gradient line at S/r = 30 and extended must cut the g axis at g = 30. The gradient for g v , or the gradient at the triangular point or below it, is (18) therefore, the approximate apparent gradient at or above the triangular point is 0.301 = 3o(l + ^~~] kv. \ Vr r) per cm. max. This follows because of the assumption of a straight line through two fixed points. SPARK-OVER 83 The approximate spark-over voltage above the triangular point is e 8 = g s r log R/r kv. to neutral max. Below the triangular point it may be found by substituting g v for g s . In Fig. 88 each drawn curve is for g 8 values calculated for vary- ing spacing at constant radius. The points are measured values. The corona boundary line is the g v curve; it intersects the # curves at S/r = 30. Corona does not form below this line, but it sparks across immediately. This is greater than the theo- retical ratio, as explained below. See also pages 2729. 300 280 260 240 .220 200 Il80 100 80 60 40 \ Spa) Sp; .05 J.O ,15 .20 .25 .30 .35 .40 .45 .50 Kadius of Wire iu cm. FIG 89. Apparent spark-over gradients for parallel wires. (Points measured, curves calculated.) In Fig. 89 each curve is drawn for a constant spacing and varying radius. The broken line is the critical ratio line. It also corresponds to the g v curve. For spacings below this line spark takes place immediately before corona forms, and the g a values fall pretty well on the g v line as shown by triangles. Fig. 90 is voltage plotted in the same way. Below the corona boundary, where spark occurs before corona, the e a curve does not hold. The broken lines are calculated from g 9 and e v . The points are observed values. Thus corona gradient and spark-over gra- dient, and hence spark voltage and corona voltage below S/r = 30 > are the same. 84 DIELECTRIC PHENOMENA No great accuracy is claimed for this formula. It may, how- ever, be useful in approximately determining the arc-over between conductors in practice. Dirt or water, however, will greatly modify the results, as will appear below. The reason that spark takes place before corona can form at small spacings or below S/r = oc is discussed on page 27 for con- centric cylinders, in which case g was taken as constant. S 180 1 160 1 140 2120 l>100 .60 I 40 ^20 \ 30 .05 .10 .15 .20 .25 .30 .35 .40 .45 - .50 JRadius of Wire m cm. FIG. 90 Spark-over voltages between parallel wires. (Maximum values to neutral given. Points measured, curves calculated.) We know, however, that g v is a function of r, and for air Q.301X Vr ) + '/- } r loge R/r Differentiating for maximum 0301X/ ""^A e R/r - 1 - 0.301A ~ or, e v is maximum when / + 0.301 0.301\ ' --J &* h ^" ~^ > S* It *" / fa /o 3* / 1 n 6 67 ( m. ( 10 n c4*ejo oo ol (N ol el Eadms of Inner Cylinder ( r ) FIG. 91. Spark-over and corona voltages for concentric cylinders with vary- ing diameter of inner cylinder. "series resistance/' or it grades or distributes the flux density. (See Fig. 91.) Taking the exact equation for parallel wires ffv = (126) -1 . cosh-i ^ S 0.301 \ 2r TV -COBh-l| Vr; r \ 2r + e* =flf Varying r for constant S == 10 it is found that e v is maximum when S/r = 6.67. Experiments show this ratio to be 30. This is probably because, at the small spacing, the corona acts as a flexible conductor which collapses and forms a point. The visual corona voltages, or the spark-over voltages below the critical ratio of S/r or J?/r, should be of practical value for 86 DIELECTRIC PHENOMENA voltage measurement on account of the accuracy at which they may be determined or calculated for different temperatures, baro- metric pressures, etc. Influence on Spark-over of Water and Oil on the Conductor Surface. Tests with oil and water on the conductor surface were made in a manner exactly similar to the dry spark-over and corona tests. In the oil tests, the surface of the wire was coated with a thin even film by means of an oiled cloth. For the wet tests, water was sprayed on the conductor surface before each reading by means of an atomizer. Figs. 50, 51 and 92 are dry, wet, and oil curves for three different sizes of wire. 160 150 HO 130 g*120 |100 2 5 80 t? 70 g 60 T*> Co 10 20 Sparing m 30 40 50 60 70 em's, between Wire Centers FIG. 92. Spark-over and visual corona for parallel wires. (Diameter, 825 cm. Polished copper. Surfaces dry, wet, and oiled. Maximum volts to neutral given.) For spark-over both water and oil have approximately the same effect. This curve tends to approach the needle-gap curve. For corona, water very greatly lowers g v . Oil lowers g v but to a much less extent than water. Where the conductor is very small the per cent, increase in diameter due to oil more than com- pensates for the lowering effect. The spark gaps which have been useful in measuring high vol- tages will now be considered. SPARK-OVER 87 The Gap as a Means of Measuring High Voltages. A gap method of measuring high voltages is often desirable in certain commercial and experimental tests. A gap measures the maxi- mum point of the voltage wave and is therefore used in many insulation tests where break- down also depends upon the maximum voltage. In most commercial tests an accuracy of 2 or 3 per cent, is sufficient. A greater accuracy can be ob- tained with the sphere gap for special work where special pre- cautions are taken. The Needle Gap. The needle gap is unreliable at high vol- tages because, due to the brush and broken-down air that pre- cedes the spark-over, variations are caused by humidity, oscil- lations, and frequency. 1 The needle gap is also incon- venient because needles must be replaced after each dis- charge; the spacing becomes FIG. 93. very large at high voltages, and the calibration varies somewhat with the sharpness of the needle. AVERAGE NEEDLE SPARK-OVER VOLTAGES No. 00 Needle, 5=1 A.I.E.E. zuu 190 180 170 160 150 140 ~130 Il20 IllO Sioo 1 9 5 80 5 70 60 50 40 30 20 10 Hu mil Lity Pe. Cent 8 f. \- 5 / // iy 1.0 fy y, / 57 V, i/ / x w r/ /, Pv ff '// / // y/ / v/* ^ fa 7 / W w 4 A */ w i f f f / < Approximate Ne&dle Gap Curves for Different Relative BLumidity 5=1 60~ 5 10 15 20 25 30 35 40 45 50 55 6C Spacing In cm. Kv eff Spacing (cm ) Kv. eff Spacing (cm ) 10 1.19 40 6.10 15 1.84 45 7 50 20 2 54 50 9 00 25 3.30 60 11 80 30 4 10 70 14 90 35 5 10 80 18.00 1 F. W. Peek, Jr., Discussion, A.LE.E., Feb., 1913. F. W. Peek, Jr., G. E. Beview, May, 1913. 88 DIELECTRIC PHENOMENA 380 360 320 300 280 8240 220 siso ol60 The effect of humidity is shown in Fig. 93, where it can be seen that a higher voltage is required to spark over a given needle gap when the humidity is high than when it is low. (Curves, Fig. 93, are intended only to illustrate this effect.) It is probable that the corona streamers in humid air cause a "fog, " and then agglom- erate the water particles, which, in effect, increase the size of the electrodes. All spark-gap curves of whatever form of gap must be cor- rected for air density that is, altitude and temperature. The spark-over of the needle gap decreases with decreasing air density but the correction is erratic and unreliable. The Sphere Gap. 1 The voltage required to spark over a given gap between spheres increases with the diameter of the spheres. Corona cannot form on spheres, or rather, the spark-over point and corona point are coincident if the spacing is not greater than the diameter of the spheres. In prac- tice a spacing as great as three times the radius may be used with- out appreciable corona. The vol- tage limit of a given sphere in high- voltage "measurements is thus reached when a gap setting greater than three times the radius is re- quired. For accurate work it is preferable to use spacings less than the diameter of the sphere. This is especially so where one sphere is grounded. A larger sphere should then be used. With this space limit the first evidence of stress is complete spark- over; corona can never form, and all of the undesirable effects and variables due to brush discharge and broken-down air are eliminated. Humidity has no measurable effect. The space factor is relatively small. Several thousand measure- ments may be made without repolishing. The curve may be calculated. The only correction is the air-density correction. This has been investigated and the results are given below. The 1 Chubb and Fortlscue, A I.E E , Feb , 1913. "The Calibration of the Sphere Gap Voltmeter/' F W. Peek, Jr., A.LE.E , Feb., 1913. "The Sphere Gap as a Means of Measuring High Voltage." F. W. Peek, Jr., G. E. Review, May, 1913. WlOO Spacing in cm FIG.* 94. Spark-over voltages of 25 cm spheres. SPARK-OVER 89 TABLE XXI. SPHEBE GAP SPAEK-OVBK VOLTAGES 6.25-cm. Spheres Spacing Kilovolts effective Om Tn Non-grounded Grounded 5 1ST 12 12 1 394 22 5 22 5 1 5 591 31 5 31 5 2.0 0.787 41.0 41.0 3 1.181 57.5 56.0 4 1 575 70 5 66.0 5 I 969 81 73.0 6 2.362 89 79 7 2.756 96,0 83.0 8 3.150 102.0 88.0 9 3 543 107.0 90.5 10 3 937 110 93.0 Each point is the average of five readings. The average variation between maximum and minimum for a given setting is less than 0.5 per cent. For the grounded case, the curves wefre made with the grounded sphere 4 to 5 diameters above ground See Table XXXIV. TABLE XXII. SPHERE GAP SPARK-OVER VOLTAGES 12.5-em. Spheres Spacing Kilovolts effective Cm. In. Non -grounded Grounded 25 0.50 1.0 098 0.197 0.394 6 5 12 22.0 6 5 12 22 1.5 2,0 3.0 591 787 1.181 31.5 41 59 31.5 iOt 59.0 4.0 5.0 6.0 1.575 1 969 2.362 76 91.0 105.0 KUL 89 102.0 7.0 8 9 2 756 3 150 3 543 118.0 130.0 141 112 120JL 128 10 12. Qu, 15.0 3 937 4 72 5 91 151.0 167.0 188 .J35 fly o 160.0 17.5 20.6 6 88 7 87 201.0 213,0 168 174 90 DIELECTRIC PHENOMENA correction is quite simple. Fig. 94 gives typical sphere-gap curves for both spheres insulated and for one sphere grounded. Tables XXI to XXV give spark-over curves for 6.25, 12.5 ? 25, 50 and 100 cm. spheres at sea level (25 jleg. C. 76 cm. barometer). TABLE XXIII. SPHERE GAP SPARK-OVER VOLTAGES 25-cm. Spheres Spacing Kilovolta effective Cm In Non-grounded Grounded 5 0.197 11 11 1.0 394 22 22 1 5 591 32 32 2 787 42 42 2 5 983 52 52 3 1 181 61 61 4 1 575 78 78 5.0 1.969 96 94 6,0 2 862 112 110 7.5 2.953 135 132 10.0 3 937 171 166 12 5 4.92 203 196 15 5 91 230 220 17 5 6 88 255 238 20 7.87 278 254 22 5 8 85 297 268 25 9 83 314 280 30 11 81 339 300 40 15 75 385 325 Calculation of Curves. The gradient or stress on the air at the sphere surface, where it is greatest, is found mathematically g = f kv./cm. (13) Where e is the applied voltage in kilovolts, X is the spacing in centimeters, / is a function of X/R and R is the radius of the sphere in centimeters, SPARK-OVER 91 TABLE XXIV. SPHEEE GAP SPARK-OVER VOLTAGES 50-cm. Spheres Spacing Kilovolts effective Cm. In Non-grounded Grounded 2 787 40 O 1 40 - 4 1 575 76 5 76 6 2 362 115 5 112 8 3 150 149 145 10 3 937 189 185 12 4 72 224 3 220 14 5 51 255 5 250 16 6 30 285 275 2 20 7 87 335.0 320 25 9 83 393 377 30 11 81 445.0 420 35 13 80 493.0 456 40 15 75 537.0 489 45 17.72 573.0 516 50 19 19 605.0 541 55 21 65 633 561 60 23 62 660.0 579 65 25 60 684 594 70 27 56 705.0 608 75 29 55 725.0 619 1 These values are calculated. 2 Spacings above 16 cm are calculated- Then |/kv./cm. where e & is the spark-over voltage and g* is the apparent strength of air. / is found mathematically and tabulated on page 27, for the non-grounded and grounded cases. For the non-grounded case we have found experimentally that g sj the apparent surface gradi- ent at spark-over, increases with decreasing radius of sphere, as g v for corona on wires increases for decreasing radius of wire. 92 DIELECTRIC PHENOMENA TABLE XXV SPHEKB GAP SPARK-OVER VOLTAGES 100-cm. Spheres These values are calculated Spacing Kilovolts effective Cm In Non-grounded Grounded 1.0 394 20 20 3.0 1 181 60 60 5 1 969 100 100 10.0 3.937 195 195 15.0 5.91 283 280 20.0 7 87 364 360 30.0 11 81 520 505 40 15 75 650 615 50 19.69 770 730 60 23.62 870 810 70.0 27.56 956 895 80 31.50 1044 956 90.0 35.43 1107 1010 100 39.37 1182 1057 110 43.35 1238 1090 120.0 47 20 1290 1133 130 51.20 1335 1160 140 55 70 1378 1189 150.0 59 10 1412 1212 For a given size of sphere, g 8 is practically constant, independent of spacing, between the limits of X = 0.54\/JK and X = 2R. The average gradient between these limits of separation is 0.54 g. , 2( 27.21 1 + -^ kv./cm. max. (a) 1 H (0 54\ 1 H -?= j kv./cm. eff. sine wave. 1 (6) The maximum variation from the average between the limits may be 2 per cent. When X is less than 0.54 Vfi, increases very rapidly because the spacing is then less than the "rupturing energy distance." 1 Above X = 3JS, g* apparently gradually increases. 1 R W. Peek, Jr., "Law of Corona III," A.I.E.E., June, 1913. SPARK-OVER 93 This increase seems only apparent and due to the shanks, sur- rounding objects, etc., better distributing the flux or lessening the flux density. When both spheres are insulated and of practical size, the change is not great within the prescribed limits. In this case the neutral of the transformer should be grounded so that spheres are at equal and opposite potential. When one sphere is grounded, however, this apparent increase of gradient is very great if the mathematical /, which does not take account of the effect of surrounding objects, is used. For this reason / was found experimentally, assuming g s constant within the limits, as it is in the non-grounded case, "and finding values of f correspond- ing to the different values of X/R. Any given value of the ratio X/R should require a constant f to keep g s constant independent of 5. This was found to check. 1 The curves may be approximately calculated thus: # (non-grounded) e * ~ g * f effective sine wave. . _ _ j^ (grounded) ~ g * fo effective sine wave. Where g a is calculated from the equation (6), and/ or/<> are found from the table on page 27 for the given X/R. These equations have been given for theoretical rather than practical reasons. Curves should be calculated only when standard measured curves can- not be obtained. Measured curves are given here. The average error, however, for curves calculated from the above equations, for 2-cm. diameter spheres and over, should not be greater then 2 per cent. The accuracy of calculations is not as great as in the case of the starting point of corona on wires. The Effect of Air Density or Altitude and Temperature: Cor- rection Factor. Practical Application. We have found that the average gradient for various air densities may be expressed (n *4\ 1 + -~p== jkv./cm. max. (0 54 \ 1 -} j= Jkv./cm. effective. where 8 is the relative air density. (See page 51.) This correc- tion does not apply for small spacings at low air density. (See page 196.) 1 /o was determined with the grounded sphere 4 to 5 diameters above ground. In practice, this may vary from 4 to 10 diameters without great error. See Table XXXIV. Voltage values in tables correspond to 4 to 5 diameters above the ground for this case. 94 DIELECTRIC PHENOMENA The standard curve may be made to apply to any given altitude by multiplying the standard curve voltage at different spaeings by the correction factor thus 19.36 19.3 I 0.54 \ h VB) aV?|^ + - 64 l = I VR + 0.54 1 ea TABLE XXVI Approximate corresponding altitude Barometer Values of a at 25 deg C for standard spheres of the following diameter, cm. Cm , Hg In, Hg Ft. 6 25 12 5 25 37.5 50 75 100 500 1,000 76.00 74.58 73.14 29 92 29 36 28 79 1 000 981 964 1 000 980 0.963 1.000 0.980 962 1 000 979 961 1 000 979 960 1 000 979 0.960 1 000 979 960 1,500 2,000 2,500 71.77 70.42 60 09 28 25 27.72 27.20 948 932 916 0.946 929 0.913 945 927 911 944 926 909 943 925 0.908 942 0.924 0.907 942 924 907 3,000 3,500 4,000 67.74 66 51 65.25 26 67 26.18 25.69 902 887 0.873 0.899 0.884 870 897 882 867 0.895 880 0.865 0.893 0.878 863 0,892 876 861 891 875 860 4,500 5,000 6,000 64.01 62 79 60.45 25 23 24 72 23 80 859 845 817 855 841 0.812 0.852 0.838 808 850 835 0.805 848 833 803 846 831 0.801 845 830 800 7,000 8,000 9,000 58.22 56.03 53.84 22.93 22 05 21.20 0.791 765 739 786 759 733 782 754 728 779 750 724 776 0.748 0.721 774 746 0.719 772 744 717 10,000 12,000 15,000 51.85 48.09 42.88 20 41 18.93 16.88 0.716 0.669 0.606 709 661 596 0.703 0.656 589 698 651 585 694 647 580 692 644 577 0.690 642 0.575 In order to avoid the trouble of calculating in practice, the factor is tabulated in .Tables XXVI and XXVII. This correc- tion is very accurate. Table XXVI gives the correction factor for different sizes of spheres at different barometric pressure and at constant temperature. When the voltage strikes across a SPARK-OVER 95 given gap the voltage, e, corresponding to the gap is found from the standard curve and multiplied by the correction factor a, or a curve may be plotted corresponding to a given barometric pressure. Thus BI ea Table XXVII gives the correction factor for various values of 5. 6 may be calculated for the given temperature and barometric pressure and correction factor then found from the table. Fig. 95 gives the standard curve for the 25-cm. sphere (non-grounded) (25 deg. C. 76 cm. bar. pressure) and curves calculated therefrom for 25 deg. G. and various barometric pressures. TABLE XXVII. CALCULATED VALUES OF a FOR DIFFERENT VALUES OF 5 ,-\ VSR + 0.54 Relative | air density i Values of a Diameter of standard spheres in em 5 6 25 12 5 25 37 5 50 75 100 50 0.55 0.60 547 594 640 535 0.583 630 527 575 623 522 570 618 0.519 567 615 517 565 613 516 564 612 0.65 0.70 0.75 686 732 777 677 0.724 771 670 718 766 665 714 762 663 711 759 661 709 757 660 708 756 80 0.85 90 821 866 910 0.816 862 908 812 859 906 0.809 857 905 807 855 904 805 854 903 804 853 902 95 1 00 1 05 956 1.000 1 044 955 1 000 1 045 954 1.000 1 046 953 1 000 1 047 952 1.000 1 048 951 1.000 1 049 951 1 000 1 049 1 10 1.092 1 092 1 094 1.095 1 096 1 097 1 098 Experimental Determination of the Effect of Air Density. The equation for the air density correction factor was determined by an extensive investigation of the spark-over of spheres in a large wooden cask arranged for exhaustion of air. This cask was built of paraffined wood and was 2.1 meters high by 1.8 meters in diameter inside. (See Fig. 96.) 96 DIELECTRIC PHENOMEN'A Tests were made by setting a given size of sphere at a given spacing, gradually exhausting the cask, and reading spark-over 2 4 6 8 10 12 14 16 18 20 Spacing cm. FIG. 95. Sphere gap spark-over voltages at various air pressures. (12.5 cm. spheres. Non-grounded. Curves calculated. Points measured.) voltage at intervals as the air pressure was changed. (Tem- perature was always read, but varied only between 16 deg. and FIG. 96. Cask for the study of the variation of spark-over and corona voltages with air pressure. 21 deg. C.) This was repeated for various spacings on spheres ranging in diameter from 2 cm. to 25 cm. At the start, the SPARK-OVER 97 possible effect of spark-overs on the succeeding ones in the cask was investigated and found to be nil or negligible* A resistance of 1 to 4 ohms per volt was used in series with the spheres. Wave shape was measured and corrected for. Voltage was read on a voltmeter coil, by step-down transformer and by ratio. Pre- cautions were taken as noted in other chapters. In order to illustrate the method of recording data, etc., a small part of the data for various spheres and spacings is given in Tables XXVIII to XXXII. Considerable data are plotted in curves, Figs. 97 to 99. The points are measured values. The drawn lines are calculated by multiplying the voltage values from the standard curves at 8 = 1, by the correction factor. TABLE XXVIII. SPHERE GAP SPARK-OVER VOLTAGES AND GRADIENT 2.54-cm. Spheres. Non-grounded Barometer 75.5 Spacing Temp. Press , cm of Hg Relative air density Kv. g, measured Cm In Eff Max. Eff. Max, 0.635 25 15 75 5 72 6 70 5 68 4 65 8 62 6 60 56.7 54 8 52.6 50.5 47.6 45 4 42 4 40 36 8 1.028 990 0.957 930 0.895 0.852 0.818 0.776 745 0.717 0.686 0.649 0.618 0.576 544 0.500 15 7 15 3 14.9 14.4 14 13 6 13.2 12 5 12.1 11.8 11 3 10.7 10 4 9.8 9 3 8.7 22.2 21 6 21 1 20 4 19 8 19.2 18 7 17.2 17 1 16.7 16 15.2 14.7 13.8 13 1 12.2 29.2 28.5 27.7 26.8 26.0 25.3 24.6 23.2 22.5 22.0 21.0 20.0 19.3 . 18.2 17.2 16.1 41.3 40 3 39 2 38 36 8 35 7 34 8 32.0 31 8 31 1 29 8 28 3 27 4 25 8 24.4 22 8 98 DIELECTRIC PHENOMENA TABLE XXIX. SPHERE GAP SPARK-OVER VOLTAGES AND GRADIENTS 5.08 Spheres. Non-grounded Spacing Relative air density Kv S* measured Cm. In Effective Maximum Effective Maximum 5.08 2 1.018 78 4 111 27 4 38 9 5 08 2 980 75 6 107 26 5 37 6 5 08 2 944 73 1 103 5 25 6 36.2 5.08 2 903 70 7 100 24 8 35 5.08 2 872 68 7 97 2 24 34.0 5 08 2 836 64 90 5 22 4 31 7 5 08 2 798 63.6 90 22 3 31 5 5 08 2 764 61.1 86 4 21 4 30 2 5 08 2 0.726 58.9 83 3 20 6 29.2 5 08 2 682 56 1 80 5 19 6 28 2 5,08 2 0,654 54 76 4 18 9 26 8 5 08 2 618 51.5 73 18 25 6 5 08 2 578 49 69 3 17 2 24 3 5 08 2 ^0 544 45 8 64.7 16 22 6 5 08 2 0.510 43.3 61.2 15 2 21.4 TABLE XXX. SPHERE GAP SPARK-OVER VOLTAGES AND GRADIENTS * 12.5-em Spheres. Non-grounded Spacing Relative air density 1 Kv. measured Cm. In Effective Maximum Effective Maximum 12.7 5 0.982 163 230 23 1 32 7 12.7 5 0.951 156 221 22 2 31.4 12.7 5 0.917 150.0 212.5 21 3 30 2 12 7 5 880 147.0 208.0 20 9 29 5 12.7 5 846 143 5 203.0 20 4 29 8 12.7 5 807 139 5 197 5 19 8 28.0 12.7 5 780 134.5 190 19.1 27.0 12.7 5 0.736 131.0 185 5 18.6 26.3 12.7 5 0,699 125.0 177.0 17.7 25.1 12.7 5, 0,666 120 5 170.0 17.1 24.2 12.7 5 637 115 5 163.0 16 4 23 1 12.7 5 598 109 5 155 15 5 22.0 12 7 5 561 104.5 147.5 14.8 21.0 12.7 5 0.541 101.0 142 5 14.3 20.2 SPARK-OVER 99 .1 .2 .3 .4 .5 .6 .7 .8 .9 1.0 Eelatlve Air Density 8 FIG. 97. Spark-over voltages at different air densities. (12 5 cm. spheres * non-grounded. Figures on curves denote spacing.) TABLE XXXI. SPHERE GAP SPARK-OVER VOLTAGES AND GRADIENTS 12.5-cm. Spheres Grounded Spacing Relative air density Kv fft measured Cm. In. Effective Maximum Effective Maximum 6 35 2 5 0.908 95 5 135 21.2 30 6 35 2 5 889 92 5 130 5 20 5 29 6 35 2 5 0.828 88 6 125 19 7 27 8 6.35 2 5 0.796 85.8 121.0 19 26.9 6 35 2 5 0.758 81.1 114 5 18 25 4 6 35 2 5 723 78 2 110.5 17 3 24 5 6.35 2 5 0.690 73 2 103 5 16.2 23.0 6 35 2.5 0.653 71.5 101 15.9 22 4 6 35 2 5 0.620 68 2 96 3 15.1 21 4 6 35 2 5 0.582 64 3 90.9 14.2 20 2 6,35 2 5 0.539 60 7 85 8 13.5 19.0 6 35 2 5 0.439 55 6 78.5 12.3 17 4 100 DIELECTRIC PHENOMENA I 16 | 14 7 .7 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 Belative Air Density $ FIG. 98. 2 4 6 8 10 12 14 16 18 20 22 24 Diameter of Spheres cnx FIG. 99. Spark-over gradients at different air densities for several sizes of spheres. (Points measured. Curves calculated from g, = 19 35(1 H -- = TABLE XXXII. SPHERE GAP SPARK-OVER VOLTAGES AND GRADIENTS 25-cm. Spheres. Non-grounded Spacing Relative air density Kv. ff measured Cm. In. Effective Maximum Effective Maximum 7.62 3 1.018 139.0 196 5 22.2 31 5 7 62 3 978 133 5 189.0 21 4 30 3 7 62 3 0.942 129.5 183.0 20 8 29 3 7.62 3 906 126 178 20 2 28 5 7 62 3 888 121 5 172.0 19 5 27 6 7 62 3 839 115 163 18.4 26.1 7.62 3 0.796 111 157 17.8 25 2 7 62 3 752 105 5 149 16 9 23 9 7 62 3 0.718 101 5 142 16.3 22 7 7.62 3 0.685 96 2 136 15 4 21 8 7.62 3 646 91 5 129.5 14.6 20 7 7 62 3 608 87 123 13.9 19 7 7.62 3 570 81.3 115 13.0 18 4 7 62 3 527 74 7 105 5 12.0 16 9 7 62 3 0.491 70.8 100.0 11.3 16.0 SPARK-OVER 101 The calculated values check the measured values closely. The equation for the correction factor was deduced from meas- ured values as follows: From a former investigation it was found that at 5 = 1 the average gradient From this investigation it was found that the average gradient at various values of d is TABLE XXXIII. AVERAGE EFFECTIVE RUPTURING GRADIENT FOR SPHERES OF SEVERAL DIAMETERS AND VARYING AIR DENSITIES Diameter of Spheres, cm. Surface Gradients Columns marked "Calc." are from, g s = 19 35 [ 1 ' 2 54 5 08 12 5 25 Meas Calc Meas, Calc Meas. Calc. Meas Calc. 1.00 28.7 28.5 25 8 25.8 24 23 4 21 9 22 2 90 26.2 26.1 23.7 23.3 21.8 21.2 19 9 20 1 0.80 24.0 23 7 21.3 21.3 19.6 19.1 17 9 18 0.70 21.3 21 2 19.0 19.0 17.4 16.9 15 7 15 9 60 18.7 18.7 16.7 16.6 15.2 14.7 13 6 13 8 50 16.1 16.1 14 6 14.3 13.0 12.5 11 6 11.7 The average measured gradients for various values of 6 are given in Table XXXIII, the calculated values from the equation are also given. The check is quite close. It should be remembered, however, that these are average values over this range of spacing and that there is a small variation at different spacings as already explained. (See Figs. 98 and 99.) Precautions against Oscillations in Testing. A non-inductive resistance of 1 or 4 ohms per volt should always be placed directly in series with the gap. For the non-grounded gap, one- half should be placed on each -side. When one gap is grounded all of the resistance should be placed on the insulated side. One 1 F. W. Peek, Jr., "Law of Corona III," A.LE.E., June, 1913. F. W. Peek, Jr., Discussion, A.I.E.E., Feb., 1913. 7 102 DIELECTRIC PHENOMENA object of the resistance is to prevent oscillations from the test piece, as a partial arc-over on a line insulator, reaching the gap. Another object is to limit the current discharge. This resist- ance is of special importance when tests are being made on appa- ratus containing inductance and capacity. If there is no resist- ance, when the gap sparks over, oscillations will be produced which will cause a very high local voltage rise over parts of the winding. If sufficient resistance is used these oscillations will be damped out. This is illustrated in Fig. 100, which shows results of a test on a high-voltage transformer. Teat Trans. H -t-ll cms ->j<-ll cms- -cms * 9 cms >f<'5 5 cms. r W 12 Ohms per Volt I U * 25 Oh ms per Volt I CJ Very S mall I 63 1 Ohm per Volt FIG. 100. Referring to Fig. 100, the high- voltage winding of the trans- former under test is short circuited and connected to one terminal of the testing transformer. The other side of the testing trans^ former is grounded. The low- voltage winding of the transformer under test is short circuited, connected to the case and ground. Voltage is gradually applied to the transformer under test until the " measuring gap" sparks over. Insulated taps, 1, 2, 3, 4, 5, are brought out at equally spaced points on the high-tension winding of the transformer under test. Auxiliary needle gaps SPARK-OVER 103 are placed between 1 and 2, 2 and 3, and 1 and 3, to measure the voltage which appears across these sections of the winding when the main measuring gap discharges. The numbers between 1-2, 2-3, and 1-3 represent the sparking distances of the local voltages caused by a discharge of the measuring gap. Four cases are given with different values of resistance o> in the main gap. When o> = 1 ohm per volt, the local oscillations are completely damped out. With small resistance in the gap, a 19-cm. spark-over causes a voltage to build up between coils 1 and 3 (which sparks over a 150-cm. gap), although the total applied voltage across the transformer is only equivalent to a 19-cm. gap. The apparatus may thus be subjected to strains far beyond reason, and either broken down or very much weakened. Water-tube resistance is the most reliable. A metallic resistance, if non-inductive and of small capacity, may be used. Carbon or graphite rods should be avoided as, although they may measure up to a very high re- sistance at low voltage, the resistance may become very low at high voltage by " coherer " action. When the tested apparatus is such that there is considerable incipient arcing before spark-over, it is better to use the sphere to determine the "equivalent" ratio of the transformer at a point in voltage below the voltage at which this arcing occurs. The sphere gap should then be widened out, the spark-over voltage measured on the low-voltage side of the transformer or in the voltmeter coil, and multiplied by this equivalent ratio. It must also be remembered that resistances do not dampen out low frequency surges resulting from a short circuit, etc. Miscellaneous Precautions. In making tests it is desirable to observe the following precautions: The shanks should not be greater in diameter than one-fifth the sphere diameter. Metal collars, etc., through which the shanks extend should be as small as practicable, and not come closer to the sphere than the gap distance at maximum opening. The effect of a large plate or plates on the shanks is given in Table XXXIV. The sphere diameter should not vary more than 0.1 per cent., and the curvature, measured by a spherometer, should not vary more than 1 per cent, from that of a true sphere of the required diameter. The spheres should be at least twice the gap setting from surroundings. This is especially important if the objects are large conducting, or semi-conducting masses. 104 DIELECTRIC PHENOMENA walls, floor, etc. Care must also be taken to so place the spheres that external fields are not superposed upon the sphere gap. This is likely to result, especially in the nongrounded case, from a large mass of resistance units or connecting leads, etc., in back of and in electrical connection with either sphere. The error may be plus or minus as indicated for the small plates in Table XXXIV. With the water tube resistance this condi- tion is not likely to obtain as the tube may be brought directly to the sphere as an extension of the shank. Great precautions TABLE XXXIV. EFFECT OF METAL PLATES ON THE SHANKS. DISTANCE TO GROUND ON ARC-OVER OF* 6.25-cM. SPHERES Per Cent. Change of Voltage Sphere gap, cm Non-grounded 5 cm. diameter plates. 6.25 cm, back of Grounded 5 cm. diameter plates. 6.25 cm. back of Both spheres One sphere Insulated sphere Grounded sphere 1 5 0.0 + 07 -0.7 3 +1 -1.0 + 1 5 -1 5 6 +2 -2 + 30 -2.0 APPROXIMATE EFFCT OF DISTANCE ABOVE GROUND WHEN ONE SPHERE Is GROUNDED Diameters of grounded sphere above ground Percentage variation from standard curves for different spacings x - 2R x = 22 R "=2 - 10.0 - 5 5 1 - 4.5 - 3.0 2 - 2 - 1.0 3 - 1 - 0.5 4 - - 0.0 5 + 05 + 0.3 6 + 1 + 0.5 * 10 + 25 + 10 20 + 2.5 + 1.0 NOTE: The spacing, X, is given in terms of radius, R, to make the correction applicable to any size of sphere The distance of the grounded sphere above ground is, for the same reason, given in terms of the sphere diameter. The ( +-) sign means that a higher voltage and 10 diameters, never under 3. Above 10 the variations in per cent error remain about the same When both spheres are insulated, with the transformer neutral at the mid point, there is practically no variation in voltage for different distances above ground. SPARK-OVER 105 are necessary at very high voltages to prevent leakage over stands, supports, etc., and to prevent corona and brush dis- charges. Unless such precautions are taken errors will result. 280 260 240 ^220 1200 glSO 4-160 140 .2120 x ^ '/' / -^ 7 *.. / ^ < ^ ^ s # M 100 80 60 40 20 "? p* i" 1 !/ 10 20 so 40 50 60 Spacing cm . 70 80 90 KX FIG. 101. Spark-over voltages between points, o, dry; A, wet; x, rain. . 25" per minute. 60 points on 1 . 25 cm. rods. Rain and Water on Sphere Surface. Figs. 101 and 102 show the effect of rain and water on points and spheres. The ratio 400 380 SCO 340 320 300 *2SO ^260 240 S220 g 200 f?160 5140 W120 100 5 10 15 20 25 ) 35 40 45 50 55 60 Go 70 75 Spacing cm. FIG. 102. Spark-over voltages between 25 cm. spheres. 1, dry; 2, wet surface; 3, rain (0.25" per min.)- of dry to rain (0.2 in. per min.) spark-over voltage for a given spacing will average about 2.5 for 6.25 to 50-cm. spheres. High Frequency, Oscillations, Imptdses. A great deal of confusion often results in discussing the effects of "high fre- quency" on insulation without differentiating between con- tinuous sine wave high frequency, oscillations, and steep wave 106 DIELECTRIC PHENOMENA front impulses. This is so because the effects may be quite dif- ferent, and are all attributed to the same cause. High frequency from an alternator, or a series of oscillations, may cause high-insulation loss, heating, and the resulting weak- ening of the insulation. Single trains of oscillations, or single impulses, may not produce heating. Energy, and therefore definite finite time, is required to rupture insulation. For a single impulse, or oscillation, where the time is limited, a greater vol- tage should be required to break down a given insulation than for continuous high frequency or for low frequency. Experiments 30 28 26 24 22 20 i* "16 I" 12 10 8 6 4 2 3U 28 26 24 a, 22 520 1 18 16 1" *t 12 3 10 8 6 4 2 X / 4 / / f A L / X. X .1 .2 .3 .4 .5 ,6 .7 8 .9 1.01.1 Spacing cm. ,1 .2 .3 .4 .5 .6 .7 .8 .9 1.0 1.1 Spacing 0204 0.6 0.8 1 l.J Time-Micro-Seconds . 106. Impulse voltage and cii cuit producing it 2 SPARK-OVER 111 frequencies the spark-over voltage is lower than the puncture voltage. For lightning or impulse both the spark-over voltage and the puncture voltage should be much higher. 1 By applying a sufficient number of impulses at voltages higher than the 60-cycle puncture voltage, an improperly designed insulator may be punctured. During the time that the air is breaking down, this overstress produces small cracks in the porcelain. The effect is cumulative. The cracks gradually extend and puncture results. This subject is, hence, of great importance. In making spark measurements it is necessary to consider the spark lag, as otherwise totally erroneous conclusions may be reached. It is therefore necessary in making spark-over measure- ments on certain apparatus to guard against this. For instance, on line insulators there is generally considerable corona discharge long before spark-over. This discharge may cause oscillation which will affect the measuring gap and cause a lower voltage to arc over given distances than normal, or cause the gap to cause higher voltages than really exist. This is eliminated in practice by the use of high resistance in the measuring gap. One investigation of impulse voltages, indicating that time and energy are necessary to rupture insulation, 2 shows that "the disruptive discharge through a dielectric requires not merely a sufficiently high voltage, but requires a definite minimum amount of m energy. v "The disruptive discharge does not occur instantly with* the application, but a finite, though usually very small, time elapses after the application of the voltage before the discharge occurs. During this time the disruptive energy is supplied to the dielectric/ 7 The disruptive energy of oil seems to be about 30 times greater than it is for air. This is further discussed in Chapter VI. Effect of Altitude on the Spark-over Voltages of Bushings, Leads, and Insulators. For non-uniform fields, as those around wires, spheres, insulators, etc., the spark-over voltage decreases at a lesser rate than the air density. The theoretical reasons for this have been given, as well as the laws for regular symmetrical electrodes, for cylinders l knd spheres. It is, however, not possible to give an exact law covering all types of leads, insulators, etc., as every part of the surface has its effect. The following curves and tables give the actual test results on leads, insulators and bushings of the standard types. .The correction factor for any other lead or insulator of the same 1 See data, appendix. 2 Hayden and Steinmetz, A.I.E.E., June, 1910. 112 DIELECTRIC PHENOMENA type may be* estimated with sufficient accuracy. When there is doubt 8 may be taken as the maximum correction. It will gen- erally be advisable to take 8 because the local corona point on leads and insulators will vary directly with 5. This is so because the corona must always start on an insulator in a field which is locally more or less uniform. The tests were made by placing the leads or insulators in the large wooden cask, already referred to, exhausting the air to approximately 8 = 0.5, gradually admitting air and taking the spark-over voltage at various densities as the air pressure in- creased. The temperature was always read and varied between 16 and 25 deg. C. At the start a number of tests were made to see if a spark-over in the cask had any effect upon the following spark-overs by ionization or otherwise. It was found that a number of spark- overs could be made in the cask with no appreciable effect. During the test, the air was always dry and the surfaces of the insulators were kept clean. TABLE XXXVIII. SUSPENSION INSULATOR Bar. cm. Vac. cm. Pressure Temp cent. 5 Kilo volts arc-over 75 4 37.4 38.0 22 0.50 121 75 4 34.3 41.1 22.0 0.54 131.0 75 4 30.0 45.4 22 60 144 75 4 26.4 49.0, 22 0.65 158.5 75 4 23.0 52.4 22 0.70 165.0 75 4 19.3 56.0 22 0.74 177.5 75,4 17.5 57.9 22.0 0.87 183.2 75 4 15.0 60 4 22.0 0.80 195 TABLE XXXIX. LEADS Correction Factor for Leads Shown in Fig 107 & (a) (&) (c) W) 1.00 1.00 1.00 1.00 1.00 0.90 92 91 0.92 . 0.92 0.80 0.83 82 0.83 85 70 74 0.72 0.75 77 60 70 65 64 66 50 61 56 54 0.57 SPARK-OVER 113 TABLE XL. POST AND PIN INSULATOBS Correction Factor for Insulators Shown In Fig. 108 8 (a) (&) (c) Post Pin 1.00 1 00 1.00 1.00 0.90 93 0.91 0.94 80 84 81 0.86 70 0.76 0.72 0.75 60 68 0.62 0.65 0.50 60 52 0.53 TABLE XLI. SUSPENSION INSULATOE Fig. 109 Correction Factor for Units in String as Follows Number of units s 1 2 3 4 5 1 00 90 80 1.00 96 91 1 00 93 84 1 00 90 80 1 00 1 00 0.70 60 0.86 80 76 66 70 60 50 72 55 . 0.50 TABLE XLII SUSPENSION INSULATOR Fig. 110 Correction Factor for Units in String as Follows Number of units s l 2 3 4 5 1.00 90 1.00 94 1 00 92 1.00 90 1.00 90 1 00 80 87 84 80 80 70 81 73 70 0.70 60 50 0.72 62 63 52 0.60 50 60 50 Table XXXVIII is a typical data sheet. Tables XXXIX- XLI give even values of 5 and the corresponding measured cor- rection factors. If the spark-over voltage is known at sea level or 5 = 1(76 cm. bar., temperature 25 deg. (X), the spark-over 114 DIELECTRIC PHENOMENA JLOW 6 d s 140 130 120 fioo I 90 80 * 60 50 40 30 20 10 > ^c ]fr /\ / / b / / { / / & / / / ^ / / / /I 1 / A * . a ^X eS f S x" A" .1 .2 .3 .4 .5 .6 .7 .8 .9 U) 1.1 Eelatisr-e Density 160 150 140 130 120 110 100 90 80 70 .2 60 M 5Q 40 30 20 10 1 c J 3PsL / c 6 p / / / ^ a a 1 Iron gtf'Cap rSIron j^JiBase / x / X J X b X^ <** S^ 1 ^ 4 5^& n^ /* d .1 .2 .3 .4 .5 .6 .7 .8 .9 1.01.1 Relative Densities FIG. 107. Variation of spark- over voltage of transformer t leads with air density. (a) 15 2 cm high by 17 8 cm. dia. (6) 21 6 cm high by 17 8 cm. dia. (c) 28 cm. high by 17 8 cm dia (d) 38 1 cm. high by 17 8 cm. dia Height measured from case to metal cap on top. FIG. 108. Variation of spark-over voltage insulators with air density. (a) 30 2 cm. high (6) 13 5cm high by 16 . 8 cm. dia. (c) 28 6 cm high by 36 cm dia. 21U 200 / 190 IRfl ky 170 160 150 (. / 1 /c > / 140 130 19H S / Arc Over Voltages at Various Air Densities .2 .3 .4 .5 .6 ,7 .8 .9 0.0 J&elatLve Density FIG. 109. Suspension insulator. (Dia., 30 cm. Spacing 16.5 cm.) Z1U 200 190 180 170 160 150 140 130 120 I 110 |ioo 1 90 ^ 80 M 70 60 50 40" SO 20 fl h j V -C: 7 ^ / / ^ ^ / $ \ / X <$$ \ ^ / * o / P ,/ ^^ E 3 / / - volts (aa .) To Neutral FIG. 115. Characteristic corona loss curve for large stranded conductor. Line A conductors 1-2-3-4. 3/0, 7-strand cable, diameter, 1 18 cm. Total conductor length, 109,500 cm. Spacing, 310 cm. Points, measured values. Curve calculated from p = 0.0117 (e 72. 2) 2 . e - Disruptive critical voltage. e v = Visual critical voltage. Test table XLIV. The values of e and p for the set of readings to be investigated are first tabulated and a curve plotted (Fig. 1 16) . All points that differ greatly from the straight line are eliminated as probably in error, or, as at the lower part of the curve, following a different law. The remaining readings are taken and formed into two groups, each of an equal number of readings. Group 1. Sie Group 2. 2 2 e 1 Steinmetz, Engineering Mathematics, page 232. 124 Then DIELECTRIC PHENOMENA where n is the number of points used. Thus e and c are determined. :40|l! 110 120 130 140J150 ICO 170 180 190 200 210 Bet Lines 55 65 e o75 85 95 105 To Neutral Kilovolts Effective FIG. 116. Corona loss curve plotted between \/p and e. Data same as Fig. 115.) (Large conductor. TABLE XLV. CORONA Loss, CALCULATED VALUES FOR FIG. 115. p - c 2 (e - e ) 2 p - 0.0117 (e - 72.2) 2 Kilovolts be- tween lanes e' Kilovolts to neutral e Kilowatts P = c 2 (e eo) 2 Kilovolts be- tween lines e f Kilovolts to neutral e Kilowatts p = C 2( e e a )2 144 4 72.2 183.2 91 6 4 41 150 75 0.10 187.0 93.5 5 32 159 79.5 63 200.0 100 9 03 165.8 82.9 1.34 209.0 104 5 12 25 169 84.5 1.77 214.2 107 1 14 25 176.6 88.3 3.04 220.2 110.1 16 80 CORONA LOSS 125 TABLE XLVI. CORONA Loss Method of Reducing (Data from Table XLIV) Kilovolts between knee' Kilovolts to neutral e Kw., p Vp 120 4 60 2 0.11 0.332 130.2 65.1 0.15 388 139 2 69.6 22 0.470 150 75.0 40 0.632 159 79.5 0.79 0.889 165 8 82.9 1.42 1.192 169.0 84.5 2 04 1.428 176.6 88.3 3 21 1.792 183.2 91.6 4.28 2.069 187.0 93 5 5 55 2 356 200 100 8 78 2.963 209.0 104 5 12 02 3.467 214 2 107.1 13.99 3.740 220 2 110.1 16 94 4.116 Total conductor length Spacing No. 3/0 seven-strand cable diameter . e Vp 91 6 2.069 93 5 2.356 100 2.963 104 2 *3.467 107.1 3 740 110.1 4.116 285.1 321.4 ASe = 36.6 AZ\/P = 3.935 SSe = 606.8 SS\/?> = 18.711 .109,500 cm. 310 cm. 1.18 cm. ASe c 1 = 0.0115 e e/ 7.388 11.323 72.1 144.2 Table XLVI shows the method of reducing. The curve, Fig. 115, is drawn from the equation p = 0*0117 (e - 72.2) 2 . The circles show the experimental values, and" indicate where the losses deviate from the quadratic law. 126 DIELECTRIC PHENOMENA -Table XL VII gives a similar set of data for a small wire. results are plotted in Figs. 117 and 118. The 7 6 5 I 4 I 3 2 1 f / 1 ( J ^ ' / / y / ^ e,v // t i o I X f \& X 20 40 60 80 100 120 140 ICO 180 200 220 10 20 30 40 50 60 70 SO^loVub 6 " Kilo- Volts Effective To Neutrftl / / 06 /* / < 'V / ; x 1 ^ / >-- * -t" 00 J20 140 ICO 130 200 22C Between Line 50 60 70 80 90 100 11 Kxlo-Volta Effective ToNeutra FIG. 120. FIG. 121. Corona loss plotted between \/p and e to illustrate the quadratic law. FIG. 120. No 8 copper wire. Diameter, 0.328 cm. Total length, 29,050 cm. Spacing, 244 cm. Temp. 1 . 5. Bar., 76 . 6. Line B. FIG. 121. 3/o, 7-strand weathered cable. Diameter, 1 . 18 cm. Spacing, 310 cm. Total length, 109,500 cm. Temp., 16. Bar., 75 3. Line A. taken up to 20 times the disruptive critical voltage, and show how well the quadratic law holds. Figs. 120 and 121 are plotted in the same way to illustrate the quadratic law. CORONA LOSS 129 Frequency. To determine the way that frequency enters into the power equation a series of loss curves were taken on line A at various frequencies. These tests indicated that the loss varied almost directly with the frequency over the range investigated. The data are given in Tables XL VIII and XLIX. Thus when the frequency does not TABLE XL VIII. LINE A. CONDUCTOR 2-3. TOTAL LENGTH 54,750 CM. Kilovolts between lines 210 200 190 180 / Kilowatts loss 47 4.9 3.2 2.0 1.3 60 5 1 3.7 2.6 1.6 70 6.1 4.3 2.8 1.7 80 6.9 5.0 3.4 1.9 3 6 2 1 90 7.5 5.6 3.8 2.6 100 8.0 5.6 3.7 2 4 115 9.3 7.1 5.0 3.4 TABLE XLIX. LINE A. CONDUCTORS 1-2-3-4. TOTAL LENGTH 109,500 CM. Kilovolts between 210 200 190 180 lines / Kilowatts loss 50 9.24 6.30 3.80 2 20 60 10 50 7.30 4.65 2.65 70 12.1 8.60 5.50 3.20 80 14.0 10.20 6.80 3.95 vary greatly from 60 cycles the equation may be written P Kilowatts km (p) V" KllovoltB neutral e Is 1 j * Kllovolts neutral e Kilowatts km. (p) ^ * 010 - / r(^ t ^ o AAQ T / e, lx* P ^ \ /| ^x S 1" * Vi ^ ^/ x^ ^ ^ ^ ^ x' x <" 004 V o .004 / X 1 r^ ^ " "-v O r / ' . ^ ^ x / Jx x- > ^ ^ -20 20 40 60 80 100 120 Frequency FIG. 123. Variation of c 2 with fre- quency. (Data from Table LI.) 1000 2000 3000 4000 6000 6000 7000 FIG. 124. Variation of c 2 with s/r. to mean for a given wire and spacing a constant loss plus a loss which varies directly as the frequency. The equation may be written p = a(/ + 25)(0-e ) 2 At zero frequency the equation reduces to p = 25a(e e ) 2 132 DIELECTRIC PHENOMENA This is not necessarily the direct-current loss but is probably lower as the maximum voltage is applied for less time. Watson has made laboratory measurements of d.c. loss, using an influence machine as the source of power. 1 Some of these measurements are compared with the a.c. loss in Table LII, for the same maxi- mum voltages; the difference between the d.c. loss and the a.c. loss for the same effective voltages is much greater. TABLE LII. COMPARISON OF D.C. CORONA Loss WITH Loss AT 60 QYCLBS FOR SAME MAXIMUM VOLTAGE Voltage gradient D.c. amps. i D.c. kilovolts e D.c. loss p kw./km. Corresponding a c. effective kilovolts ei Measured 60 -cycle loss Pi kw /km. Ratio 60 cycles d c loss pi P ei 0.003 55 16 39.8 0.25 1.52 66 0.004 59 0.24 42.0 37 1 58 69 0.005 62 31 44.0 50 1.61 75 0.007 67 0.47 48.0 80 1 67 s = 100 cm. r = 0.0597 cm. D.c. measurements from Watson, Institute of Electrical Engineers. Relation between c 2 and s/r. The power equation may be written over the commercial range of frequency p = c 2 (e - e ) 2 = a(f + 25) (e - *) where the relation between c 2 and s/r has not to this point been investigated. The relation will first be determined for the prac- tical sizes of conductors at practical spacings of the outdoor line, and later over greater range from the indoor data. Only 60- cycle values will be used, as the data at this frequency are very complete. In Table LIII are values of c 2 for various sizes of wire and cable at various spacings. c 2 varies greatly with the radius of the conductor r and the spacing s. Plotting s/r ^nd c 2 a curve is obtained that suggests a hyperbola. The curve between log c 2 and log s/r is a straight line. Therefore the follow- ing relation between c 2 and s/r is established. = A (s/r) d (33) The fair weather value of c 2 for standard line A 1-2-3-4 may now be examined in Table LI V. 1 Watson, Journal Institution of Electrical Engineers, June, 1910. CORONA LOSS 133 TABLE LIII. EXPERIMENTAL VALUES LINES A AND B Relation between C 2 and s/r Test No Diameter, cm 5 T g c* X 105 Style of | per km ! conductor Material 95 168 6550 1.07 280 Wire Gal. iron 92 0.168 4880 1.07 256 Wire Gal. iron 86 0.168 3700 1 08 326 Wire Gal. iron 138 0.328 2980 1 10 331 Wire Copper 94 168 2730 1 07 410 Wire Gal. iron 137 0.328 2230 1 10 391 Wire Copper 91 0.168 1820 1 07 506 Wire Gal. iron 128 518 1530 1 05 412 Wire Copper 136 328 1490 1 10 513 Wire Copper 82 585 1480 1 07 513 Cable Gal. iron 135 328 1120 1 10 570 Wire Copper 94a 168 1090 1 07 633 Wire Gal. iron 77 585 1060 1.07 543 Cable Gal. iron 79 585 770 1 08 571 Cable Gal. iron 134 328 740 1.10 772 Wire Copper 126 518 700 1.11 687 Wire Copper 18 1 181 525 1 02 950 Cable Copper 80 585 520 1 07 784 Cable Gal iron 125 518 350 1 11 1070 Wire Copper 73 585 310 1.07 1018 Cable Gal iron 100 953 193 1 08 1584 Cable Gal. iron TABLE LIV. RELATION OF c 2 TO 7 FOR MAIN EXPERIMENTAL LINES o Line A 1-2-3-4 (Standard Line A) Test No. c* X 105 per km 1 ~s 8 Test No C2 X 105 per km i s 8 18 945 982 1.020 103 980 901 1 112 36 1050 966 1.037 104 892 878 1 138 37 945 959 1.043 105 890 866 1 158 84 945 933 1.074 109 869 928 1 078 101 955 925 1.081 119 991 888 1 127 It is seen that these values are not exactly constant but appar- ently vary with the temperature and barometric pressure, c 2 and 1/8 in curve, Fig. 125, suggest that c 2 varies as 1/d. Multi- plying by d then, reduces c 2 to the standard temperature of 25 134 DIELECTRIC PHENOMENA TABLE LV (Corrected c 2 and s/r) Teat No Diam- eter, cm s/r c 2 X 105 read per km corrected to 25 C , 76 cm Corr factor 5 corrected to 25 C , 76 cm s Style of conductor bar bar. 95 168 6550 280 300 1 07 5 704 8 787 Wire 92 0.168 4880 256 275 1 07 5.620 8 492 Wire 86 0.168 3700 326 347 1 08 5.852 8.215 Wire 138 328 2980 331 364 1 09 5 892 8.000 Wire 137 328 2230 391 429' 1.09 6 062 7.709 Wire 77 585 1060 543 582 1 07 6 372 6 966 Cable 126 518 700 687 755 1 10 6.637 6.551 Wire 18 1 181 525 950 965 1.02 6.821 6.263 Cable 80 585 520 784 840 1.07 6.733 6.254 Cable 125 0.518 350 1070 1190 1.11 7.083 5.858 Wire 73 . 0.585 310 1018 1090 1.07 6.995 5.763 Cable 100 953 193 1584 1710 1.08 7.405 5 263 Cable .020 FIG. 125. Relation between c 2 and 1/5. TABLE LVI. SA REDUCTION OF RELATION OF c 2 TO - r (c 2 Corrected to 25 deg. C. 76 cm. Barometric Pressure) Test No loge (C 2 1Q5) s Iog - Test No. log* (C2106) s 10g 95 5.704 8.787 126 6.637 6 551 92 5.620 8.492 18 6 871 6 263 86 5.852 8.215 80 6.733 6 254 138 5 892 8.000 125 7.083 5 858 137 6 062 7.709 73 6 995 5 736 77 6.372 6 966 100 7 444 5 263 35 502 48.169 41 763 35 925 CORONA LOSS 135 Silog (c 2 10 5 ) = 35.50 S 2 log (c 2 10 s ) * 41.76 AS Ioge(c 2 10 5 ) = -6.26 51 loge - = 48.17 5 2 loge = 35.92 AS loge-= 1225 SS Iog(c 2 10 5 ) = 77 26 SS loge ~ 84.09 AS log (c 2 10 5 ) - <2SS log. - c i _ r . n log (c 2 10 5 ) = -0.5 loge - + 9 92 c 2 = 20,500 \/-10- 5 9.92 deg. C. and 76 cm. barometric pressure. This particular correc- tion is not satisfactory as the range of 8 is small. It seems the best until more complete data are obtained. In Table LV all values of c are corrected to 25 deg. C. and 76 cm. barometer, and the constants calculated by the SA method in Table LVI. This gives: c 2 = 20,500v / 7'7s X 10" 5 per km. of total conductor at 25 deg. C. 3 76 cm. barometer and 60 cycles. Curve 124 is plotted from the points calculated in Table LVII, while the circles show the actual experimental points. TABLE LVIL CALCULATION OF CXJRVE No. 124 FROM X 105 = 20,500 0,500^) 8 T $ c 2 X IQs 5 T 4 c 2 X 10 250 0.0633 129 2000 0.0224 460 500 0.0447 915 3000 0.0183 376 1000 0.0316 648 4000 0158 324 1500 0258 530 6000 0128 262 Curve 126 shows a straight-line relation between log sfr and log c 2 . The equation for the power loss at 25 deg. C. and 76 cm. barometric pressure and any frequency may now be written p = 241(/ (34) 136 DIELECTRIC PHENOMENA where p = the energy loss per kilometer of conductor in kilo- watts. e kilovolts to neutral. e = disruptive critical kilovolts to neutral at 25 deg. C. and 76 cm. barometric pressure. / = the frequency in cycles per second. r = the radius of the conductor in cm. s = the distance between conductor centers in cm. and The value of e varies with the radius of the conductor r, the spacing s, and will be discussed later. Relation between c 2 , and r and s for Small Conductors and Small Spacings. (Indoor Line). The loss was investigated for very small conductors at large and small spacings, and for large conductors at small spacings, on the indoor line. The conductors ranged from 0.025 cm. to 0.46 cm. in radius, and the FIG. 126. Determination of equation between 6 2 and s/r spacings from 12.5 to 275 cm. This investigation is, hence, an extension of the above investigation beyond the practical range. The quadratic law still holds the relation between c 2 , r and s, however, becomes more complicated. This is also true of the disruptive critical voltage. Below a spacing of about 15 cm. it is difficult to express the loss in terms of a law, as the results are erratic, probably due to the great distortion of the field which is augmented when the corona starts, greatly increasing the loss above the quadratic. For conductors 0.025 cm. in radius and above, and 15 cm. spacing and above, this data shows that c 2 = 20,500. r + - + 04 10~ 6 per km. of conductor (33o) CORONA LOSS 137 The more complete equation is, therefore, p = 241 C/ + 25), r + - + 0.04 - e d } % 10~ 5 kw./km of conductor 1 50 40 W 30 W20 10 In Fig. 127 the points are measured corona loss values, while the curve is calculated from equation (34a) (r = 032, spacings 46 and 275 cm.). Data are given in the appendix. It is interesting to note from (33a) that as r becomes very small the c 2 term, at a given spacing, approaches a con- stant value somewhat as if the corona diameter acts as the conductor diameter. The Disruptive Critical Voltage. The point of greatest stress around a cylin- drical conductor is at its sur- face. When s/r is large the gradient at the surface of the conductor may be expressed de e I 2 20 40 60 80 100 6 - K. V. to Neutral 120 y ~ dx where e (12c) r log* s/r = the voltage to neutral. s = distance between conductor centers. r = the radius. FIG. 127. Comparison of calculat- ed and measured corona loss for small conductors at small and large spacings. (Points measured. Curves calculated from equation (34a) Conductor radius, 032 cm. Spacings, 46 cm. and 275 cm. 5 = 1 01.) When r arid s are in centimeters and e is in kilovolts, g is ex- pressed in kilovolts per centimeter. If e , which has been called the disruptive critical voltage, is taken for e, ~ r log e s/r g then is the stress at the conductor surface corresponding to e , and will be called the disruptive gradient, to distinguish it from the visual gradient g v . Values of g for wires and cables taken under a variety of conditions on the outdoor line are given in Tables LVIII and LIX. These values are corrected to standard tem- perature and pressure by dividing by d. 1 F. W. Peek, Jr., High Voltage Engineering, Journal Franklin Institute, -Dec., 1913. 138 DIELECTRIC PHENOMENA TABLE LVIII. DISRUPTIVE CRITICAL VOLTAGE GRADIENT FOR WIRES (Values Corrected to 76 cm. Barometer and 25 deg. C., Outdoor Line) Test No Spacing, cm Radius, cm g kv /cm max Per cent variation from mean Per cent variation max to mm 91 152 084 31 3 94 229 31 6 92 410 29 1 95 550 36 5 Avg. = 30 9 5 8 7 9 134 122.0 164 28 8 135 183 27 1 * 136 244 29 137 366 25 7 138 488 25 3 Avg. 27.2 7 12.7 125 91.4 259 28 7 126 183.0 26 5 127 275.0 26.0 128 397.0 26.2 Avg. = 26.9 6 7 9 4 122 91 4 0.463 28.7 123 183.0 30.4 120 214.0 . . 30.5 124 275.0 31.0 Avg. 30 1 4 8 7.6 Total Avg 29 If the values of e for standard line A (1.8 cm. seven-strand cable) are examined it is found that the average value of g is 25.8 kv. per centimeter maximum. For cables between 0.583 cm. and 1.18 cm. in diameter and various spacings, the average value of g is 25.6 kv. per centimeter maximum, or, in other words, g is constant for commercial sizes of cables, at practical spacings, and is 25.6 kv. per centimeter maximum. In determining the value g for seven-strand cables r was taken for convenience as the outside radius. Hence the above g is not the actual g as ob- tained for wires, but is an apparent g . The actual g may be CORONA LOSS 139 obtained by taking some mean radius r 2 between the outside radius r and the radius to the point of contact of the outside strands TV r 2 approaches r in value as the number of strands is increased. TABLE LIX DISRUPTIVE CRITICAL VOLTAGE GRADIENT FOR CABLES (Values Corrected to 76 cm. Bar. and 25 deg. C , Outdoor Line) Test No Spacing, cm Radius, cm | g kv /cm i max Per cent variation from mean Per cent variation max to min 73 91 4 292 26.5 80 152 24.0 79 244.0 23.9 77 310.0 23 9 82 432 25 Avg. = 24 7 7 3 9 8 100 91 4 0.476 25.5 115 91 4 26.2 116 183 26.0 117 275 26 4 118 366 28 1 Avg. = 26 4 6 4 9 3 Line A - 1. 2. 3. 4 18 310 590 25 5 36 310.0 26 37 310.0 25 3 84 310.0 25 8 101 310.0 26 5 103 310.0 26 1 104 310.0 25 7 105 310.0 26 . . 109 310.0 25.8 119 310.0 25 1 119 310 26 Avg. = 25 8 2 7 5 3 Total Avg. = 25 7 5 5 8 1 The values of g for wires varying in diameter from 0.168 cm. to 0.928 cm. and for spacings from 90 to 600 cm. are constant within the limits of experimental error. This more than covers the commercial range. The mean max. value is: g = 29 kv. per cm. at 25 deg. C., and 76 cm. barometric pressure. 140 DIELECTRIC PHENOMENA Considerable variation should be expected in g values obtained on a long outdoor line, due to 1. Necessarily imperfect conductors, kinks, etc., in an outdoor line of this length. 2. Progressive change in the value of successive points on a given curve due to slight changes of wave shape, etc., as the vol- tages are increased, and the apparent shift of e . The close agreement of g for wires is for the above reasons remarkable. Discrepancies due to progressive change are not to be expected for standard line A to any great extent as the conductor spacing was always the same, and test conditions were kept as nearly constant as possible. g ou iuo M 30 I 20 iw c3 o flr 29.8 N Avgi x X _o 7e 25.7 Avgr, X * a= Wir Gab 3S les 1234 567 Badius in cms FIG. 128.- . 90 for wires and cables. (Data from Tables LVIII and LIX ) The above data shows that g may be considered constant for diameters of conductors and spacings within the practical range. This immediately suggests that g is the actual rupturing gra- dient of air or identical with g of the expression for visual corona. This was further investigated over a greater range on the indoor line. g cables - - : -- = m g wires where m is a fraction which approaches unity as the irregularity of the surface is reduced, or number of strands increased. Then e = dm g r log* s/r (See curve, Fig. 128.) The loss equation may now be written (35) P = ~ e o? 10-* fcw./km. (34) CORONA LOSS 141 where p expresses the loss above the visual critical voltage e v , and e is given in (35). Investigations on the indoor line over a range covering small conductors show that the disruptive gradient may be considered for all practical purposes, constant when the conductor radius is greater than 0,20 cm. As the size of the conductor is decreased the disruptive gradient increases very rapidly. If the disruptive gradient for any size of conductor is called g d we have found that this law may be expressed: t . 0.30 1 \ 1 + ^ f ^^ ^ } (36) (1 + 230 r 2 ) e d = g d r log, - (35a) .2 .3 .4 .5 .6 .7 B&dius in cm. .8 .9 FIG. 129. Comparison of g v , g&, and g . values from Table LX.) Thus, when r is large (above 0.2 cm.) practically g d = g<>, and where r = o, g d = g v > This apparent increase in disruptive gradient for small con- ductors gives the impression that the residual from the very highly ionized air resulting at each cycle in effect increases the size of the conductor. Thus, the g d formula is the same as the g v formula with the energy distance term apparently modified or lessened by the residual ionization at each cycle, g <> results for large conduct- ors. Measured values of g d for different conductors on the indoor line are given in Table LX. Calculated and measured values are plotted in Fig. 129. The corona loss equation over a greater range of conductor diameter and spacing may thus be written 142 DIELECTRIC PHENOMENA r + - + 0.04 p = 241(/ + 25)^ S (e - e where e d is obtained from equation (35a). TABLE LX 10~ 5 kw./km. (34o) Test No r cm gd maximum measured gd maximum calculated 12 B 032 67 5 70 7 13 B 0.032 70 3 70 7 14 B 032 71 70 7 18 B 032 71 70 7 15 B 032 71 70 7 16 B 032 71 70 7 19 B 032 69 6 70 7 17 B 032 71 2 70 7 20 B 032 69 5 70 7 21 B 032 69 3 ?0 7 Avg -70 27 B 057 51 7 51 3 26 B 057 51 3 51,3 25 B 057 51 7 51 3 24 B 0.057 51 3 51 3 Avg. =51 5 30 B 071 45 4 45 4 33 B 0914 39 4 39 4 32 B 0914 39 4 39 4 42 B 105 42 2 37 6 41 B 105 42 2 37 6 37 B 105 42 5 37.6 Avg -42 3 45 B 164 36 5 * 33 44 B 164 33 6 33.0 Avg. =35 1 49 B 256 30 8 31 1 48 B 256 32 1 31.1 47 B 0.256 33 2 31.1 Avg, =32 56 B 464 31,8 , 30 2 55 B 464 31 8 30 2 54 B 464 31 5 30 2 Avg. =31 7 CORONA LOSS 143 It may be interesting to note that equation (34) may be written in terms of the gradient, thus (/ + 25) (log ) 2 (r 2 ) (g - g o y X 10~ 5 p Fig. 130 shows measured curves plotted between g and p for a given wire at three different spacings. These curves all intersect the axis at g max. = 30, at d = 1.0. 4.U 3.5 3.0 I 2 - 5 ^2.0 gl.5 1&X.O .5 < w ? ,oM ^> >^ ^ 3*^, " <& ^ ^ Test Nos * . 94 xxx 94 A ooo 95 Diam = .168 cm *& ^ ' ^ ^ ^., [' ;s*- 10 20 30 40 50 60 70 80 90 100 110 120 ISO 140 150 ICO 170 180 Apparent Surface Gradient FIG 130 Relation between power loss and apparent surface gradient. Losses Near the Disruptive Critical Voltage e Q . If the con- ductors could be made perfect no appreciable loss would occur below the visual critical voltage. However, near the starting point of corona two effects occur, which cause a deviation of the loss from the quadratic law, equation (34), and which affect the loss in opposite directions: (a) With perfect conductors loss of power does not begin, at the voltage e 0) at which the disruptive gradient is reached at the conductor surface, but only after the disruptive strength of air has been exceeded over a finite and appreciable distance a from the conductor, that is, at a higher voltage e v . Since the con- vergency of the lines of dielectric force is great at the surface of small conductors, with such conductors, a considerable increase of the voltage is required to extend the disruptive gradient to some distance from the conductor, and e v is considerably higher than e . With such conductors there would be no loss until e v were reached. The loss would then suddenly take nearly the definite value calculated for this applied voltage from equation (34). Even with polished conductors, in practice the decrease of loss below that given by equation 34 is appreciable with small conductors within the range between e and e v , as seen in Fig. 131. 144 DIELECTRIC PHENOMENA With large conductors, however, the less convergency of the lines of dielectric force at the conductor surface requires a less voltage increase beyond e to extend the disruptive gradient to some distance from the conductor; e and e v are therefore closer together, and this decrease of the loss below the theoretical value given by equation (34) is not appreciable. (6) As the conductor sur- face can never be perfect, some loss of power occurs at and below the disruptive criti- cal voltage at isolated points of the conductor, where irreg- ularities of the surface, scratches, spots of mud or dirt, etc., give a higher poten- tial gradient than that corre- sponding to the curvature of 2.2 2.0 1.8 1,6 1.4 ftA2 H ,6 .4 .2 E / 1 I 1 1 I I/ / / / 1 isurec Loss / / / Qutid ~0022 ratic P'o / / f- X^ _ ^' 60 80 100 12 Between Line 20 30 40 50 6 Kilovolts Effective To ^utral FIG. 131. Corona loss for small con- ductors near the critical voltage. No. 8 copper. Diameter, .328 cm. Length, 29,050 cm. Spacing, 122 cm. Temp 1 5. Bar., 76 6. Line B. the conductor surface, appreciable, since the curvature of the con- ductor surface is of the same magnitude as that of its irregu- larities. It becomes appreciable, however, for larger conductors, as seen in Fig. 132. This excess of the loss beyond that given by the quadratic law equation essentially depends on the con- ductor surface, and is the larger the rougher or dirtier the surf ace is. With small conductors, this loss is rarely 100 110 120 130 140 150 160 170 180 190 200 _ A - A Between Lines 50 60 70 80 90 100 Kilovolts Effective To Neutral J'IG. 132. Corona loss for large conductors near the critical voltage. (Data same as Fig 115.) It is a maximum at the disruptive critical CORONA LOSS 145 voltage e oj and decreases above and below e v , and is with fair accuracy represented by the probability curve: where q is a coefficient depending on the number of spots, and h is a coefficient depending upon the size of spots. Snow, sleet and rain losses seem to be of the same nature, but frequently of far greater magnitude. * Equation (37) is probably of no practical importance as the loss is small, and q and h naturally cover a wide range of values, depending upon the condition of the conductor surface. Experi- mental values near e are taken from Table XLIV and tabulated in Table LXI, together with values calculated by the quadratic law. Corresponding experimental and calculated values are subtracted and also tabulated. TABLE LXI LINE A 1-2-3-4 FROM TABLE XLIV, TEST 36 c 2 = 0.0117 e = 72 2 Kolovolts between conductors e f Kw exp Po Kw p = 00117(e - e*)2 Excess loss Pi = (Po P) log* pi (e - e) 2 120 4 11 11 2.40 146 5 130 2 15 15 2 71 49 139 2 22 22 3 09 6 2 150 40 10 30 3 40 8 5 159.0 79 63 16 2 77 54.7 165 8 1 42 1 34 08 2 10 11 7 Fig. 132 is plotted to a large scale to show the excess loss near e . As this is for large conductors, e and e v are near together, and the effect of (&) predominates. In order to see if equation (37) holds, write log e pi = log q h(e e) 2 Then the curve between log pi and (e e) 2 should be a straight line. This is shown in Fig. 133. Values of q and h are of the following order for Line A : Test No q per cm. total conductor h 30 3 19 X 10~ 6 0.0220 105 2 47 X 10~ 6 0,0208 103 2 74 X 10~ 6 0304 146 DIELECTRIC PHENOMENA Fig. 131 is plotted from values for a small smooth conductor. Here e and e v are far apart, and as the curvature of the conductor surface is of the same magnitude as its irregularities they do not greatly influence the loss. The (a) effect here predomi- nates that is, the loss near e c is lower than that shown by the quadratic law. 1 The loss between e and e v is iftistable as it depends upon surface conditions. In all 50 75 100 125 150 FIG. 133. Determination of equa- tion (37). cases the quadratic law is closely followed above e v , and on large practical sizes of con- ductors with sufficient accuracy over the whole range. Temperature and Barometric Pressure. Values of the dis- ruptive critical voltage e covering a considerable temperature range are tabulated in Table LXII. Correction is made to a TABLE LXII. TEMPERATURE AND DISRUPTIVE CRITICAL VOLTAGE e (Standard Line A 1-2-3-4) Test No Temperature Bar cm e'okv bet lms e' corr to 76 cm 1/V Weather Wet Dry 18 16 18 5 75 5 138 5 140 0.00715 Bright sun. 15 20.0 22 75 2 140 142 0,00705 Cloudy sun 37 10 13.0 75.7 141 142 00705 Bright sun 36 iao 12 75 144 2 146 5 00683 Cloudy 109 -3 -2 73 9 148 8 150 8 00663 Hazy sun 84 1 3.0 75 2 149.0 151 00662 Cloudy 101 -1 -1 74 7 153 8 156 8 00638 Cloudy 103 -4 9 -4 5 75 7 155 3 156.7 0.00638 Sun 104 -9 5 -9 5 76 2 157 157 00637 Sun 119 -6 5 -6 76 5 156 6 156 1 00642 Sun 105 -13 -13 76.2 161 161.0 00622 Sun barometric pressure of 76 cm. on the assumption that e' varies directly with the pressure. In Fig. 134 l/e' is plotted with temperature. The straight line through these points cuts the temperature axis at 273 deg. C. or absolute zero. Temperature was always measured in the shade. The points that do not fall 1 This condition is likely to obtain to a greater extent at high altitudes as e and e v are farther apart. CORONA LOSS 147 well on the curve are the summer sunny day points. This is what would be expected, as the conductors were at a higher tem- perature than the temperature read. Fig. 134 shows that the disruptive critical voltage or the dis- ruptive gradient varies inversely as the air density. The data range, however, is not great. The density of air at 25 deg. C. and 76 cm. barometric pressure is taken as the standard. Humidity, Smoke, Wind. Humidity. Line A was kept as a standard throughout the tests. A careful study of the disruptive critical voltage and , c 2 shows no appreciable effect of either humidity or " vapor ^ .7 / ^1 .6 / .5 *.s 5ii .2 .1 -2 / / / / x 1 / > . ^ /** y |~ 240 200 160 120 80 40 , + 40 6( Degrees C. FIG. e . 134 Effect of temperature on (Data from Table LXII.) products." 1 (See Table LXIII.) Visual tests, made on two short parallel wires indoors over a great humidity range, also bear this out. TABLE LXIII STANDARD LINE A. 2 CONDUCTORS 1-2-3-4 Test No Temperature Relative humidity Vapor product go reduced to 25 deg C , 76 cm bar Wet Dry 15 20.0 22 84 55 18 8 18 16 18 5 75 35 18.5 36 10 12 78 0.25 18.8 37 10 13 67 21 18 3 84 1 3 69 11 18.7 101 -1 -1 1 00 17 19 2 103 -4 9 -4 9 1 00 0.13 18,9 104 -9 5 -9 5 1 00 08 18 6 105 -13 -13 1 00 0.06 18 8 109 -2 -2 1.00 0.12 18 7 Theoretically there should be no appreciable effect of humidity 1 Mershon, High Voltage Measurements at Niagara, A.I.E.E., June 30, 1908. 2 Line A was kept at constant test conditions for use as a standard in the study of varying atmospheric conditions, etc. 148 DIELECTRIC PHENOMENA on e , since even if the water vapor, which may be considered as a gas dissolved in air, has a different disruptive gradient than air, the percentage of the gas in the mixture should be too small to cause any appreciable change. It has been suggested that "vapor products" is a measure of ionization and, in that way, the critical voltage varies with vapor products. This does not seem likely, because with all ordinary atmospheric air the per- centage of ionization is so v small that it would not be expected to produce any effect. To test this, the visual critical point was determined on two parallel wires. The room was then closed and the wires were run at a point very much above this critical point for about an hour, or until a very intense odor of ozone filled the room. The voltage was then removed and the surface of the wires cleaned in order to remove oxidization. The critical point was then redetermined and found to be the same, although the amount of ionized air was many times that which could be expected in free atmospheric air. Of course if the percentage of ionization were great enough, as for instance in an ozone machine, a change in the disruptive strength would then be expected. It has been claimed that ultraviolet light reduces the sparking point. This is not borne out in tests, where any quantity of continuously applied power is involved. Though ultraviolet light, ionized air, and various radiations cause the small energy in condensers to discharge when applied over comparatively great time ; in case of large energy discharge in a very short time, as spark discharge, and corona due to continuously applied voltages, no appreciable effect should be expected, or can be observed, since the discharge which takes place by ionized air is not of the same order of magnitude as that produced by the spark discharge. The time required for a given voltage to pro- duce ionic saturation or discharge, should, however, be less with high initial ionization than with low initial, ionization. Hence for impulse voltages of steep wave front and short duration, the spark voltage may be affected by initial ionization. This is further discussed in Chapters IV and VIII (page 198). It is quite probable that humidity has some slight effect on the loss after corona has once formed due to the change of the gas into vapor and the agglomeration of the water particles by the ions. This is noticed in the spark-over between needle points at very high voltage. In this case there is a very heavy brlzsh discharge before spark-over. The sparking voltage increases CORONA LOSS 149 with increasing humidity, due to the fog formed, when there is not a mixture of two gases, air and water vapor, as in the case where humidity is concerned, but actual water particles are in the air. Steinmetz has observed that fog actually raises the striking distance between needle points. The effect of humidity on the spark discharge observed by the author is discussed in Chapter IV. Greater loss should be expected in corona measurements during fog due to charge and discharge of the water particles. This causes loss at lower voltages and has the effect of decreasing the critical point. While humidity has no effect on the starting point of corona, an effect might be expected on the loss after the discharge had already started. The 'reason that this is inappreciable is because the corona discharge from wires covers very little space, Smoke. It was difficult to get measurements to show the effect of smoke, as the prevailing winds were over the fields toward the city. At one time, however, during a change in the wind thick smoke was blown over the line from smoke stacks of a fac- tory, and the loss was increased. This, however, will probably not be a serious consideration in practice. Wind. Losses measured during very heavy winds show no variation from losses measured during calm weather. That the losses do increase with increasing air velocity has been shown in laboratory apparatus. There is, however, no appreciable effect due to the comparatively low air velocity in practice. Moisture, Frost, Fog, Sleet, Rain and Snow. During some of the first tests it was noted that the losses were sometimes greater on the "gomg-up curve" than on the " coming-down curve/ 7 especially in the early mornings after heavy dew. The losses became less after the line had been operated for a while at high voltage. Fig. 135 shows this well for a conductor with a coating of frost. This excess loss was thought at first to be due to leakage through moisture on the insulators. Insulators were put up without line wires, but measurements showed a very small insulation loss even during storms. It was then concluded to be due to moisture on the conductors themselves. Visual tests made on short lengths of wet and dry cables showed this in a very striking manner. Two parallel dry cables were brought up to the critical point. Water then thrown on the cables. What had been a glow on the surface of the dry cables now became, at the wet spots, a discharge extending as much as 5 to 8 cm. 10 150 DIELECTRIC PHENOMENA from the cable surface. T^l *ipT/' i am 4n /A if This discharge reminded one of an il- luminated atomizer Illustrations, Figs. 67 and 68 show this, but a greater part of the effect is lost in reproduction The wires became quite dry and down to normal discharge after running at high voltage for a 100110 120 130140 Bo ICO 170 ISO 190 200 210220230240 Bet Lines ao eo 70 so so ioo no 120 TO Neutral very few minutes. Kilo.Yolts Effective FIG. 135 Corona loss with frosty and dry conductors (Conductor length, 109,500 cm. Spacing, 310 cm Diameter, 1 18 cm 3/0,7-strand cable. Line A. Temp , -2 C. Bar , 74 cm.) and free water particles in the air. The curves, Pig. 136, taken during the fog also show the ^combined effect of condensed moisture on the cables. The moisture particles on Kflo-Volto FIG. 136. Corona loss during fog; conductors wet. (Conductor length, 109,500 cm. Diameter, 1.18 cm. Spacing, 310 cm. 3/0,7-strand cable. Line A. Temp , 2. Bar., 75.5.) 18 17 16 ,15 14 13 12 in 2Z ^_ Kilo-Yolta Elfcctivo Eto. 137. Corona loss during snow storm. (Conductor length, 109,500 cm. Diameter, 1.18 cm. Spacing, 310 cm. 3/0,7-strand cable. Line A. Temp., 0. Bar., 74.2.) the conductor become charges and are repelled. The particles CORONA LOSS 151 in the air also become charged and discharged thus increasing the loss very greatly above that for dry conductors. The losses during snow and rain storms are much greater than fair weather losses at the same temperature and barometric 90 100 110 120 130 140 150 160 170 180 190 200 210 220 230 Kilo Volts Effective FIG 138. Corona loss during sleet storm. (Conductor length, 109,500 cm. Diameter, 1 18 cm Spacing, 310 cm. 3/0,7-strand cable. Line A. Temp ,-10. Bar., 75 4.) pressure. In Fig. 137 the actual measured loss is plotted, and also a corresponding calculated fair weather loss. The difference between the two curves shows the excess loss due to snow. The effect of snow is greater than that of any other storm condition. This is because the particles are larger and a greater num- ber strike the line, or come near the line. The sleet curves are of special interest. Sleet had already started to form on the conductors, and was still falling when the tests were started. Fig. 138 shows the loss curves. After the curves were taken S 7 a ' E?6 A Kilo-Volts Effective FIG. 139. Corona loss with sleet on the wires. (Conductor length, 109,500 cm. Diameter, 1 18 cm. Spacing, 310 cm. 3/0,7-strand cable. Line A. Temp. 10 0. Bar, 76.) the line was kept at 200,000 volts for over an hour with no apparent diminution of sleet. This seems to show that sleet will form on high- voltage trans- mission lines. The day after these tests were made was bright and clear and the conductors were still coated with sleet. A set of readings was taken, and it is interesting to note that the excess loss here is as great as when sleet was falling. (See Fig. 139.) 152 DIELECTRIC PHENOMENA The excess loss for sleet, rain or snow storms (over the fair weather loss) seems with increasing voltage to approach a maxi- mum and then to decrease again (the latter at a value very far above the disruptive critical voltage), and the curves of loss seem to have the general shape of the probability curve, as is to be expected theoretically. The above readings show the im- portance of taking weather conditions into account in the design of high- voltage transmission lines. Very High Frequency. Corona losses at very high frequency are diffi- cult to measure. The curve in Fig. 140 is interesting. The drawn curve is calculated from formula 34 (a) ; the points are measured values. Power was supplied from an Alexanderson 100,000-cycle alternator. The power was measured by adjusting reactance and capacity until unity power factor The watts input was 600 400 M 300 200 / Curve Calculated 1 Points Measured V / 1 1 1* 1 1 V * f/ s 100 50 14 16 18 20 22 24 26 28 30 Kilo-Volts Elfective.Between. Lines FIG. 140. Corona loss at high frequency. (Two parallel wires Spacing, 67 cm. Radius of was obtained, wire, 127 cm / - 100,000 Total length, 200 cm.) then the product of volts and amperes Tests by Alexanderson. as measured by hot wire meters. This good check seems to show that the formula applies over a large range, but complete conclusions cannot be drawn from this small amount of data. CHAPTER VI CORONA AND SPARK-OVER IN OIL AND LIQUID INSULATIONS The most common liquid insulation is transformer oil obtained by fractional distillation of petroleum. This oil has various characteristics, as flashing point, freezing point, viscosity, etc., depending upon the specific use to which it is to be put. The average characteristics of transformer oil are as follows: 1 Medium Light Flashing temperature 180-190 C 130-140 C. Burning temperature 205-215 C. 140-150 C. Freezing point. . . -10 15 -15 20 Specific gravity at 13 5 deg. C 865-0 870 845-0 850 Viscosity at 40 deg.C. (Saybolb test) 100-110 sec. 40-50 sec Acid, alkali, sulphur, moisture None None Various other oils are insulators, as gasoline and cylinder oil; animal oils, as fish oil ; vegetable oils, as linseed oil, nut oil, china wood oil, etc. All of these when pure have the same order of dielectric strength. The so-called compounds made by dissolving solid gums in oil to increase viscosity are generally unreliable, unless used dry as varnish. Under the dielectric field the dielectrics of different permittivities tend to separate, and there is considerable loss. As in air there is very little loss in pure oil until local rupture, that is, brush discharge or corona, occurs. The dielectric strengths of oils are usually compared by noting the spark-over voltage between two parallel brass discs 1.25 cm. in diameter, and 0.5 cm. separation. The spark-over voltage for good oils in the above gap should be between 50 and 70 kv. maximum, and hence, if the voltage wave is a sine, from 35 to 50 kv. effective. 2 Different Electrodes. In Fig. 141 are plotted spark-over curves for different electrodes in good transformer oil. The character- 1 Tobey, Dielectric Strength of Oil, A.I E.E , June, 1910 2 The breakdown voltage of oil like that of air depends upon the maximum point of the wave. 153 154 DIELECTRIC PHENOMENA istics are very much the same as for air excepting the apparent strength is very much higher. Effect of Moisture. The slightest trace of moisture in oil greatly reduces its dielectric strength. The effect of moisture is shown in Fig. 142 (a) for the standard disc gap. Water is held in suspension in oil in minute drops. When voltage is applied 300 280 260 240 220 200 180 SlGO uo 120 100 80 60 40 20 / A cm Sphe res (1 )ia^ / / / / xd 10 lOrr cm. E .r>m iiscs cmE dgea' / / / S / / / 1.1 ) cm (D Sphc ia) res / / / / '/ /* t*. edlQS 1 // [/ 1 / s / / fl / / 1 / / 1 / s ' / / (Tei ip. 2 0> 1234 5678 9 10 Spacing cm FIG. 141. Spark-over of various shaped electrodes in oil at 60 *v these drops are attracted by the dielectric field. Thus they are attracted to the denser portions of the field and may form larger drops by collision. When attracted to, and after touching a metal part, ancl thus having the same potential, they are imme- diately repelled. If the field is uniform the drops form in conduct- ing chains along the lines of force. It can be seen that the effect of moisture should vary greatly with the shape of the electrode, and with some shapes the moisture may even be removed from the space between the electrodes by the action of the field, in which case its presence would not be detected by low-voltage breakdowns. In fact, for needle points and most electrodes at large spacing the breakdown voltage for wet and dry oil is practically the same. In transformers moisture will generally be CORONA AND SPARK-OVER IN INSULATIONS 155 attracted to points under greatest stress. The most effective way of removing moisture is by filtration through blotting paper. Dirt in oil may have an effect very similar to moisture and the small conducting particles be made to bridge between electrodes by the dielectric field. Solid barriers are effective in preventing the complete lining up of moisture particles between electrodes. While they generally do not increase the puncture voltage for dry oil, they very greatly increase reliability in apparatus. Sep page 189. See appendix. Temperature. Temperature over the operating range has very little influence on the strength of oil. The strength increases at the freezing point. The curve is shown in Fig. 142(6). The insulation resistance is also shown. The increase in strength (a) (b) jg 70 PLATE (Distance of wire from plate = 16.5 cm. at 60 ~) Kv eff Radius wire, cm, 0v kv /cm eff . 0* kv/cm. max. 50 0.025 278 393 60 0.050 185 262 80 0.0635 201 284 100 0.1520 122 173 55 00508 615 870 158 DIELECTRIC PHENOMENA corona voltages up to fairly high ratios of R/r are the same, and may be used in determining the strength of oil. TABLE LXVIL SPARK-OVER VOLTAGES FOR No. 6 TRANSIL OIL CON- CENTRIC CYLINDERS R cm. r cm Kv eff Kv max g s max kv /cm 1 Vr R T Remarks 3 81 032 45 3 64 420 5 61 120 00 Tests made in 3 81 238 60 84 8 127 7 2 05 16 00 long cylinders 3 81 317 60 5 85 5 108 1 1 77 12 00 with belled 3.81 0.635 69 5 98 3 86 3 1 26 6 00 ends. Oil be- tween standard 3 81 794 75.0 106.1 85.5 1.12 4 80 discs 5 cm. 3 81 952 73 103 2 78.1 1 02 4.00 apart tested 58 3 81 1,111 76.7 108 5 79.4 95 kv. (max ) 25 3.81 1 270 76 107 5 77.0 89 3 00 deg. C 3 81 1 587 73 7 104 3 75 1 79 2 40 3 81 1 905 66 3 93 7 70 7 72 2 05 3 81 2.540 45 5 64 3 62 4 63 1 57 6 67 5 560 29 2 41 3 40 6 Tests made on 6 67 5.080 43 7 61 8 44 8 short cylinders 6 67 3 970 70 1 99 2 48 1 where field is 6 67 3.240 84 4 119 5 51 somewhat dis- 6 67 2 230 105 8 149 7 61 2 torted. 6 67 1 955 105 148 5 61 9 6 67 1.615 103 5 146 5 64 6.67 1 270 101 3 143 2 67 5 6 67 953 98.3 139 75 6 67 635 94 133 89 2 6 67 477 91 5 129 5 102.8 6 67 0.318 85 3 120 7 121,0 6 67 159 65 2 92.2 155 5 6 67 079 62 2 88 251 4 11.42 3.930 144 203 5 48.3 11.42 2 280 163.0 230.4 63 11 42 1.910 158 223 2 64.5 11.42 1 270 160 226.0 81 5 11.42 880 148.0 209 93.0 11 42 520 90.0 127 3 79 5 The strength of oil for different sizes of wire from Table LXVII is plotted in Fig. 143. The curve is similar to that for corona in air. Fig. 144 shows that a straight line relation holds approxi- CORONA AND SPARK-OVER IN INSULATIONS 159 mately between ~F and g v . Values are not used when R/r > 3.5. Thus, as in the case of air: 1 1-2 g v = 36( 1 + 7=)kv./cm. max. g v = 25.5 1 + 1.2\ kv./cm. effective sine wave. 200 180 glGO gioo .4 .8 1.2 1.6 2.0 2.4 2.8 3.2 Eadius-cm FIG. 143. Strength of oil at 60 /v, (Concentric cylinders g v at surface of inner cylinder.) zoo 180 B 16 ^40 ^120 J 100 t 60 40 20 ^ ^ ^ <^ V ^ ^ ^5 ^"^ & 4* j* j^. * ^ **^ ' 04 8 1.2 1.6 2.0 2.4 2.8 3.2 3. FIG. 144. Strength of oil at 60 ~. (Method of reducing values given in Fig. 143 to equation.) The energy distance is 1.2\/r or almost four times that of air, indicating that a greater amount of energy is required to rupture oil, or a greater number of collisions are necessary before ionic 1 F. W. Peek, Jr., High Voltage Engineering, Journal Franklin Institute, Dec., 1913. 160 DIELECTRIC PHENOMENA saturation is reached. g and a vary to a considerable extent in oil. The strength of oil, or the disruptive gradient, or the gradi- ent required to bring the ions up to collision velocity, seems fairly low. Oil should, therefore, have low strength in bulk, but high Gradient H: V. cm. (^far.) \ \ V s* ~-t * =a ? 5te= ft -1 )0 1 2 3 4 Spacing cm. FIG. 145. Showing increase of strength of oil at small spacmgs at 60 (Spheres, R = 3 33 cm.) 3t>U OOA OAA OQA M * oo 220 '. 200 1 t> W 160 S 14.0 \ 1AA ^ ^ ort ^ "^^ h ~^. ^^^ Rf) -. "-^~ "- , Aft "^-^ 20 1 2 3 4 5 6 7 8 9 10 11 12 18 Eadius-cm. FIG. 146. Strength of oil between spheres at 60 ~. (Data from constant part of the curve.) apparent strength when sub-divided or confined to make use of the large energy distance necessary to rupture. Spark-over voltages and gradients are given for various spheres CORONA AND SPARK-OVER IN INSULATIONS 161 at various spacings in Table LXIV. The characteristics of the curves between gradient and spacing are the same as those for air (see Fig. 42) as shown in Fig. 145. When the spacing is so small that it interferes with the energy distance the apparent strength of oil increases. At spacings above this the gradient is constant until the separation is so great that corona forms before spark-over. TABLE LXVIII. SPHEEES IN OIL Gradient at constant part of the curve Tests at 60 Data from Table LXIV Radius, cm Gradient, kv /cm max l VR Radius, cm Gradient, kv /cm. max i VR 159 348 2 51 1 27 120 89 237 260 2 05 3 12 98 0.56 355 222 1 68 6 25 82 40 555 169 1 35 12 50 56 0.28 The rupturing gradient at the constant part of the curve for various spheres is given in Table LXVIII, and is shown in Fig. 146. This may be written approximately kv./cm. max. g. = 28.3 1 + The energy distance is approximately 2\/R. The spark-over voltages for concentric cylinders, where R/r< about 5, and for spheres above 2\/R spacing on the constant part of the curve, may be approximated by substituting g in the voltage formula T? e = g v r log* cylinders (useg v , p. 159) X e - g -j spheres (use g s above) In oil, the apparent strength can be greatly improved by limiting the free energy distance by barriers, etc. This can be seen in Tables LXIV and LXV, where e/X is given for parallel planes, and g v for spheres. For the small spacings, where the free energy distance is limited, the apparent rupturing gradient is very high, 162 DIELECTRIC PHENOMENA just as in the case of air. Strengths as high as 700 kv./cm. have been reached. Insulation barriers give an added effect by pre- venting moisture particles from lining up. Care must be taken, however, that the barriers are not so placed as to increase the stress on the oil by the high permit- tivity of the solid insulation. Transient Voltages. Transient voltages or impulse voltages of short duration greatly in excess of the low frequency rupturing voltages may be applied to insulations without rupture. In other words, the rupture of insulation requires not only a suf- Above circuit used by author A is sparked-over by transformer voltage C then discharges through L, arc at A, and R Impulse appears across R, at /. The power arc at A is non-oscillatory and, in effect, a switch The impulse voltage is determined by C, Land R FIG 147. "Impulse" circuits. ficiently high voltage, but also a definite minimum amount of energy. This means also that a definite but very small time elapses between the application of voltage and breakdown. This is sometimes called the " dielectric spark lag" and has already been discussed for air in Chapter IV. 1 The rupturing energy seems to be much greater for oil than for air, as indicated by the large energy distance in the gradient equation above. At low frequency a given definite voltage is required to cause iPeek, "The Effect of Transient Voltages on Dielectrics," A.I.E.E. Trans., 1915, page 1857. CORONA AND SPARK-OVER IN INSULATIONS 163 rupture during the comparatively unlimited time of application. This voltage is constant until the application is limited to a definite minimum time, when a higher voltage is required to accomplish the same results in limited time. Such transient voltages of short duration, and impulses of steep wave front, must not be confused with continuously applied high frequency where breakdown will generally take place at lower voltages, due to loss, etc. In Table LXIX the relative breakdown voltages of gaps in oil, at 60 cycles, and for impulse voltages of steep wave front, are given. An impulse voltage much higher than the 60-cycle vol- tage is required to break down a given gap. If similar air and oil gaps are set to rupture at the same low frequency voltage, a much higher transient voltage will be required to rupture the oil gap than the air gap, indicating greater time. An air gap may thus protect an oil gap, but not vice versa. See page 108 and appendix. TABLE LXIX. COMPARISON OF 60-CYCLE AND IMPULSE SPARK-OVER IN OIL AND IN AIR Oil Air Gap Spacing, cm Kv 60 cy , max Kv im- pulse, Gap Spacing, cm. Kv 60 cy , max Kv im- pulse, max max Stand, disc. 5 56 6 170 2/0 needles. . 1 50 2 103 3 2/0 5 1 50 2 67 8 2.0 68 8 157 needles 17 5 108 198 3 89.2 233 3 4 108 321 25 37 2 117 3 2.54-cm. 51 62 8 199 4 spheres. 77 87 5 279 1 02 111 2 337.0 6 25-cm 25 47 5 162 5 spheres. 51 68 3 244 5 70 88 3 267 1 02 115 8 284 The above voltages are measured by sphere gaps at low fre- quency and for impulse. The difference between the 60 cycles and impulse voltages increases as the steepness of the im- pulse increases. Fig, 147 shows impulse circuits. Fig. 14:7(1)), 164 DIELECTRIC PHENOMENA 8.4 A 7 R 1 7 2 1 6 8 /CO 6 4 / 6.0 5.6 5.2 4.8 .4.4 4.0 3.6 3.2 2,8 2.4 2.0 1.6 1.2 0.8 0.4 / / / ^ I X X 4.C i x x i / ^x "3. )0 1 / x" 1 / / x ^* -2. w 1 / / / ^ x^ / / / x // / 00 i. 1 // ^~- -~"""" / r r. - .50 fi ""^ teL D 10 20 30 40 50 60 70 80 90 100 1 Kilo -Volts FIG. 148. Needles in air. 2.1 2.0 1.9 1.8 1.7 1.6 1.5 1.4 1.3 1.2 1.1 S1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 / / / X ***' 00 / 1.0 / / / / ^, - / / / X 3.0 I / / / ^ I / / S x" 2.0 / / X S / f 1 / / '/, 'A / / l/\ / // // //// ^ ^-*- 1.0 // '// x* ^ i / // --a, Is? / '/ . - . - -* - X*" _ :ss" .25 ) 10 20 30 40 50 60 70 80 90 1001 Kilo-Volts FIG 149. Spheres in air. (Transient voltages. Limited energy.) 0.95 0.90 0.85 0.80 0.75 0.70 0.65 0.60 0.55 EJ0.50 0.45 0.40 0.35 0.30 0.25 0.20 0.15 0.10 0.05 1 1 1 1 (X f / \ / '4.0 \ / f \ / \ / \ / / / / 1 1 x o 1 / X y ' 1 / / / / / / - =sm M ^ X xl ^ *~~ ~ ~0 10 20 30 40 50 60 70 80 90 100 Kilo.Volta Fio, 150. Needles in oil. (Transient voltages, 0.38 0.36 0.34 0.32 0.30 0.28 0.26 0.24 0.22 0.20 0.18 0.16 0.14 0.12 0.10 0.08 0.06 0.04 0.02 / I / 1 1 oo j 1 1 I 1 1 / X^ ^ ' to 1 x^ ^ 1 S ' r-I^** *-*-*" 2.0 / / x^ ^- - " T"b~- I/ X ^-*- ---- 7: XX ^-" . =SS .50 /" 10 20 30 40 50 60 70 80 90 100 Kilo-Volta FIG. 151, Spheres in oil, Limited < CORONA AND SPARK-OVER IN INSULATIONS 165 however, does not give a circuit for which the constants can be definitely calculated. Oil is an excellent insulation in combina- tion with barriers. On solid insulations the effect of transient voltages is cumulative. A partial break occurs which is en- larged by each succeeding impulse, until finally dynamic follows. With oil, such "cracks" are closed up by new oil immediately. One investigation shows that when the energy is limited a voltage is reached where the spark distance becomes a function of the energy and practically independent of the voltage. 1 Figs. 148, 149, 150, 151 taken from this investigation show the spark- over curves for oil and air. The figures on the curves represent the current allowed to enter in the impulse, and thus indirectly indicate, to a certain extent, the energy. The impulse was produced by suddenly applying a continuous voltage to the low side of a transformer (Fig. 147b). The curve marked oo is for infinite energy supply (60 cycles). If sphere gaps are set in air and in oil for 30 kv. at 60 cycles the spacings are 0.95 cm. and 0.16 cm. respectively. If a transient voltage of 100 kv. is applied, the gap in oil will not spark over if the energy applied to the circuit is less than 1.04 joules (4 amp.). For air the minimum energy is 0.45 joule (1.5 amp.). At continuously applied high frequency oil breaks down at lower voltages than at 60 cycles. The following comparison made by the author is of interest. TRANSIL OIL BETWEEN FLAT TERMINALS SQUARE EDGE 2 5-CM. DI- AMETER 0.25-CM. SPACE BREAKDOWN VOLTAGE GRADIENTS 60 cycles High frequency alternator 90,000 cycles Single impulse, sine shape, corresponding to 200,000 cycles Kv./mm. (max.) "Kv./mm. (max.) Kv /mm. (max ) 17 6.7 39 D.C. Strength of Oil. 2 The d.c. strength of oil generally corresponds to the maximum (\/2 X effective) 60 ~ value. 1 Hayden and Stemmetz, Transactions A.I.E.E., June, 1910. 2 Peek, " The Effect of High Continuous Voltages on Air, Oil and Solid Insulation/' A.LE.E., 1916. n CHAPTER VII SOLID INSULATIONS General. Some of the principal solid insulations are varnished cambric, oiled and varnished pressboard, built up pressboard, treated wood, mica, micanite, soft and hard rubber, synthetic resins, glass, and porcelain. With gaseous and liquid insulations as air and pure oil there is very little loss up to the breakdown gradient. A gradient just under the breakdown gradient may be applied and held and the loss is so small that no appreciable heating results. Thus, the loss in air and oil is essentially a phenomenon above the electric elastic limit. This loss generally exists in some locally broken down part of the insulation, as the corona on the surface of a wire. The break does not extend through the whole insulation, and when the stress is removed, new air takes the place of the broken down air and all evidence of overstress is removed; in other words, in air and oil a local breakdown is "self healing. 77 Almost all insulations are partially conducting or have a very high resistance which is spoken of as insulation resistance. The actual resistance of the insulation itself, which is very high, apparently has no direct connection with the dielectric strength, which is measured by the gradient or flux density or stress re- quired to electrically strain the dielectric above the " electrical elastic limit " so that actual rupture or breakdown occurs. For instance, in a condenser made of two metal plates with a solid dielectric between them, when a.c. potential is applied, energy is stored in the dielectric by electric displacement at increasing potential and delivered back to the circuit at decreasing potential, as long as the potential does not stress the insulation above the elastic limit. If the dielectric were perfect a wattmeter in the circuit would indicate no loss. In all practical insulations the wattmeter does read a loss due to the PR loss in the insulation, and the dielectric loss, sometimes called dielectric hysteresis. 1 If the voltage is sufficiently increased to exceed the elastic limit actual rupture or breakdown occurs; along this discharge path the insulation is destroyed. Air has a very high insulation 1 In what follows the total loss will be called the dielectric loss. See pages 36, 37. 166 SOLID INSULATIONS 167 resistance, but not a very high dielectric strength. When the insulation resistance, however, of a given solid insulation becomes very low, as caused by moisture, etc., it is an indica- tion of large loss and low breakdown voltage. Thus, the term " insulation resistance" generally takes into account the resist- ance of the occluded moisture. Insulation Resistance. The actual resistance of the insulating material itself is generally very high. Practically all solid and liquid insulations absorb moisture to a greater or less extent. The capillary tubes and microscopic interstices, etc., in the struc- ture become filled with moisture and gases. In the non-homo- geneous structure this makes a complicated arrangement of ca- (b) FIG 152 Diagrammatic representation of resistance arrangement in imperfect insulations pacities and resistances in series and in multiple. A simplified diagrammatic illustration of the distribution is shown in Fig. 152. Let 152 (a) represent a magnified section of insulation between two terminals, and 152(6) a diagrammatic representation. The resistance of the insulation itself, which is very high, may be represented by r t . 1 may be a moist fiber which extends only partially through the insulation and is thus in series with a capacity. It may be represented by r a . 3 and 4 may be wet fibers which extend all the way across, and are represented by r m . There may also be leakage resistance over the surface. Direct current is used to measure insulation resistance, as the charging current for a.c. is very large and masks the resistance current. Watt measurements are necessary, as well as volts and amperes, to determine the effective a.c. resistance. The a.c. and 168 DIELECTRIC PHENOMENA d.c. resistance should, however, be quite different. When d.c. is used sufficient time must elapse after the application of voltage to allow for absorption (see Chapter II, page 36) . With d.c. the only path for the current is through r % and r m in multiple, which is, therefore, the resistance measured. The resistance varies with the applied potential, decreasing with in- creasing potential. The conducting particles are caused to line up, cohere, occluded gases break-down, etc., as the potential is increased. When a.c. voltage is applied to insulation the capacity current must pass through r a ] in shunt with this is the circuit through r t and r m . The loss in r a must increase with increasing frequency, while the loss through r % and r m must remain constant at a given voltage, independent of the frequency. The greater loss will generally occur in r a . The d.c. insulation resistance cannot be used in approximating the IV a.c. loss. If the a.c. loss is meas- ured, as well as the voltage and current, the effective resistance may be calculated. This resistance loss, however, must be greater than that due to 7 a as other losses are included. In. Table LXX some d.c. resistances are given for different materials. Note the effect of moisture absorbed from the air even for varnished materials. TABLE LXX. INSULATION RESISTANCE Resistance Megohms per Cm. Cube (Data obtained by Evershed, J.I.E E., Dec. 15, 1913) DC volts 50 100 200 500 Cotton, dry Cotton not dried. 350 2 8 275.0 2 5 200.0 2 2 140 Micamte, exposed to air , . ]VIicanite dried 220.0 * 175,0 160 300,000 140 200,000 Cylinder oil, trace of moisture Cylinder oil dry 22,000 36,000 22,000 36,000 22,000 36,000 Varnished cloth, 12 hr. after baking. Varnished cloth, 9 days after baking 17,000 35,000 14,000 35,000 11,000 35,000 9,000 SOLID INSULATIONS 169 With air and oil an appreciable loss begins only when a definite gradient, sufficiently large to cause local rupture as brush or corona, somewhere results; loss occurs after the elastic limit has been exceeded. The dielectric loss in solid dielectrics is essen- tially a loss below the elastic limit. In solid dielectrics a stress may be applied lower than the elastic limit, which after a short time on account of the heating and hence weakening of the insulation will cause rupture. Rupturing Gradients. Apply voltage lower than the puncture voltage between concentric cylinders with dry insulation between surfaces, and gradually increase to the rupturing voltage within a short time so that there can be no appreciable rise in temperature. The mechanism of rupture will be quite different for oil or air, glass or porcelain, and cambric. For oil and air corona results near the surface of the inner cylinder, the breakdown is local, and disappears 100 3 ! 5 \ \ \ V 05 10 15 20 25 30 35 4C Time Minutes FIG 153. Insulation puncture voltage vs. time. (Oiled pressboard, 2 5 mm thick. The curve does not cut the kv axes as it appears to on account of the time scale.) when the stress is removed; or, if the stress is further increased spark-over finally results. For glass or porcelain, as soon as over- stress is reached locally, a crack results at the surface of the inner cylinder and complete breakdown follows. With cambric there is local rupture and local charring of the insulation, which forms carbon " needles. 77 The break is progressively increased; this continues until the breakdown is complete. A wet thread or gas bubble, as (1) in Fig. 152 (a), may, in effect, act as a needle and thus cause breakdown. The breakdown gradients of solid insulations are thus variable and not as definite as with air and oil. The puncture tests on solid insulations vary greatly between different samples of the same material, shape and area of the electrodes, time of application of voltage, etc. Insulations should be thoroughly dried before tests are made. 170 DIELECTRIC PHENOMENA la comparing solid insulations it is generally best to make some arbitrary time tests to include the effect of dielectric loss, and thus, heating on the breakdown voltage. The effect of loss is cumulative; the insulation becomes warm and while the loss increases with the temperature, the dielectric strength generally decreases with increasing temperature. The ultimate strength naturally, then, depends on the rate at which this heat is con- ducted away. This is illustrated in Fig. 153. With the electrode used, if the voltage is " rapidly applied" before heating occurs, 80 kv. are required to cause rupture. 1 If 50 kv. are applied rupture does not occur until 4 minutes have elapsed, while 30 kv. may be applied indefinitely without rupture if the room tem- perature is not increased. The curve does not cut the voltage axes as appears in the cut, on account of the time scale, but is an asymptote to it. The effect of temperature is also illustrated in Table LXXI, where, in one case, the electrode is of brass giving good heat conduction, and in the other case of wood coated with tin-foil giving poor heat conduction. As the applied voltage approaches the "rapidly applied" rupturing voltage there is not sufficient time for the insulation to heat to a great extent and the effect is about the same for either brass or the coated wood electrode. The effect of heating is also shown by, d.c. tests, page 191. TABLE LXXI, EFFECT OF HEAT CONDUCTING PROPERTIES OF TERMINALS ON TIME OF BREAKDOWN Two Thicknesses of No. 12 Oiled Cloth (From Rayner, Journal LE.E,, Feb. 8, 1912) V-lic, Time of breakdown Brass terminals Wood terminals 2 9,000 570.0 sec. 50,0 sec. 10,000 48.0 sec. 19 . sec. 11,000 16 5 sec. 10,0 sec. 12,000 10. 2 sec. 6 2 sec. 14,000 5 . 2 sec. 4 5 sec. 1 Rapidly applied voltage as used above means voltage applied within a fairly short time, a few seconds, and not impulse voltage or voltage of very steep wave v front. "Instantaneous" is commonly used to designate this test; this term is confusing. The test itself is not wholly satisfactory as it is indefinite. It offers, however, a means of making a preliminary com- parison of insulations. 2 Coated with tin-foil. SOLID INSULATIONS 171 The effect of applying a high voltage, allowing different periods of rest for cooling, and then applying voltage until rupture, is shown in Table LXXIL The injurious effects of applying high voltage for different lengths of time is shown in Table LXXIIL This is probably due to the effect of heat and injury to the sur- face by corona. TABLE LXXIL RECOVERY IN VARYING PERIODS OF REST AFTER APPLI- CATION OF 9000 VOLTS FOR 1 MINUTE l Two Thicknesses of No. 12 Oiled Cloth (From Raynor, Journal I.E.E., Feb. 8, 1912) Period of rest Time to break at 11,000 volts Period of rest Time to break at 11,000 volts 1 mm 2 6 sec. 9 5 sec 5 sec 2.5 sec. 4 4 sec 2 min Fresh material. . 11 9 sec. 12 sec. 15 sec. 60 sec. Fresh material 9 Osec. 9 8 sec. 20 5 sec TABLE LXXIII (From Raynor, Journal LE.E , Feb. 8, 1912) Time of treatment at Time of breakdown ( left to cool over night) 5000 volts At 6500 volts At 7000 volts o 22 min. 8.5 min. 1 hr . . 6 5 min. 8 3 sec. 2 hr 3 sec. TABLE LXXIV. EFFECT OF AIR GAP (CORONA) Two Thicknesses of No. 12 Oiled Cloth 10,000 Volts (Raynor, Journal I E.E., Feb. 8, 1912) Air gap, mm. 0.00 30 0.50 75 1.05 Time to puncture, seconds 42 34.0 27.5 24 120 (irregular) 1 TSme to break at 9000 volts, l-# to 2 minutes. 172 DIELECTRIC PHENOMENA The action of corona or breakdown of the air at the surface of the insulation is shown in Table LXXIV. The arbitrary practical tests for comparing insulations are the Rapidly Applied (Instantaneous) Test, the One-minute Test, and the Endurance Test. Rapidly applied breakdown voltage is found by applying a fairly low voltage and rapidly increasing until breakdown occurs. Voltage should be increased at about 5 kv. per sec. The Minute Test is made by applying 40 per cent, of the rapidly applied voltage, and increasing this voltage 10 per cent, at 1- minute periods until puncture occurs. (Total time about 5 min.) The Endurance Test is made by applying 40 per cent, of the minute test voltage and increasing the voltage 10 per cent, every hour or half hour until puncture occurs. These tests may be made at any given temperature. The electrode should be of a given size and weight. Ten-centimeter diameter electrodes, slightly rounded at the edges, will be found convenient. Table LXXV gives an example of such tests. TABLE LXXV Muslin with Three Coats Varnish Total Thickness 2 mm. Rapidly Applied (Instantaneous) Breakdown and Resistance Temp , cleg Resistance in megohms for samples cent 1 2 3 4 5 20 73,400 73,400 97,900 97,900 73,400 75 650 390 310 270 170 100 100 90 73 70 50 Breakdowns in kilovolts. Tests made in oven at 100 C. 100 40.6 42 44 43 36 5 Average breakdown 40.6 kilovolts One-minute Test Apply 40 Per Cent of Rapidly Applied Breakdown Voltage for 1 Minute, with 10 Per Cent. Increase in Voltage Each Minute Temp , deg Resistance in megohms cent. 6 7 8 9 10 20 73,400 73,400 73,400 97,900 97,900 75 320 333 451 274 330 100 50 60 70 40 60 SOLID INSULATIONS 173 Time under stress Potential applied Temperature for samples 6 7 8 9 10 Air Start 100 100 101 103 100 100 1 min 16,000 101 101 103 104 102 100 2 mm 17,500 102 102 104 105 103 100 3 min 19,000 105 104 106 108 105 100 4 min 20,500 111 108 108 111 107 100 5 min . 22,000 121 112 111 117 108 100 5 min 5 sec 23,500 115 punctured 5 mm 46 sec 23,500 146 punctured 6 min 23,500 118 114 129 100 6 mm 10 sec 25,000 135 punctured . . . . 6 mm 35 sec 25,000 118 punctured . . . . 7 min 135 100 7 min 58 sec. 26,500 140 punctured 1 Endurance Test Apply 40 Per Cent, of 1-minute Period Endurance Voltage, for 30-mmute Periods Endurance Test, with 10 Per Cent. Raise in Voltage Each Period Temp , deg Resistance in megohms cent 11 12 13 14 15 22 74,300 74,400 74,400 99,100 49500 75 390 420 230 290 110 100 90 70 30 60 30 Time under stress Potential applied Temperature 11 12 13 14 15 Air Start 0.5 hr.. 34 min. 54 min. 1 hr. 1.5 hr. . 2hr 2 hr. 23 min 2 hr 25 mm . 2.5 hr. 3hr.. .. . 3 hr. 2 min 10,000 11,000 11,000 11,000 12,000 13,000 14,000 14,000 14,000 15,000 16,000 99 103 104 106 106 136 143 145 r 100 107 108 111 118 203 f 100 133 182 p 101 108 uncturec $9 115 I .. . 198 pi mctured 100 100 mctured 100 100 100 mnctui 112 114 122 215 pi ed . mnctui I ed . 174 DIELECTRIC PHENOMENA A considerable amount of data is given here for the 1-minute time test. It must be remembered that in design only a fraction of the maximum gradient corresponding to this voltage is per- missible for continuous operation, the particular per cent, depend- ing upon the design, the insulation, the rapidity at which heat may be radiated, or conducted away, etc. It is generally 10 to 15 per cent, on main insulation; it is often as low as 5 per cent., sometimes as high as 30 per cent. Strength vs. Thickness. Insulation tests are generally made for convenience on sheets between flat terminals. The gradient at the edges, even when these are rounded, is generally higher than the average gradient e/x. This edge effect is differ- ent with different thicknesses of insulation. The puncture voltage per centimeter thick- ness is always greater for thin sheets of insulation than for thick ones. This is partly due to the edge effect which cannot be corrected for and becomes relatively greater as -the thick- ness of insulation is increased. (At small spacing^ e/x is very nearly the true gradient; at large spacings e/x is not the true maximum, gradient.) l It is also greatly due, in the time tests, to the better heat distri- bution and dissipation in the thin sheets and partly due to the fact that energy is necessary for disruption, so that when the rupturing distance is limited, as in the case of thin sheets, the apparent strength increases. Fig. 154 shows apparent variation in strength with thickness. Be- tween parallel plates the apparent strength is approximately: 880 860 840 820 800 280 260 g -240 220 &200 |l80 %160 140 120 100 80 60 40 20 A \ \ \ \ \ \ s, \_ \ N 'v X, ^v "-> 1 . *--*. "". J .04 .06 .08 .10 .12 .14 .16 .18 .20.22 .24.26.28 Thickness- cm FIG. 154. Insulation strength vs. thickness. flfc = where g and a are constants and t is thickness. When shielded edges are used, it is generally best to make in- sulation tests under oil unless it is desired to make a study of the 1 Special flat terminals are sometimes used with "shielded" edges so that e/x is the true gradient. INSULATIONS 175 effect of corona on the insulation. With pointed electrodes the in- stantaneous puncture voltage of a given insulation will be less in oil than in air. This is not because the oil weakens the insulation but because corona forms on the point in air and spreads over the surface giving the effect of a fiat plate electrode. Solid and Laminated Insulation. The structure of most insu- lations is not homogeneous. If a given insulation is tested with terminals of varying area it is found that the average puncture voltage becomes lower as the area is increased, and thus the chance of it covering a weak spot is increased. As would be expected this approximately follows the probability law as shown in Fig. 155. Disruptive Voltage-Kilo FO Its s s \ Pn babi ifcyC urve X A V ^^ Exj erlra euta Cur 7fi 1234 Radius of .Flat ermiaals-Gm* 10 18 10 15 20 12 FIG. 155. Insulation strength vs area FIG 156. Variation in di- of terminal. electric strength at different parts of a piece of insulation. The reason that the experimental curve bends down is that the gradient is fairly constant until the terminal becomes small when the gradient increases, due to flux concentration with the smaller terminal. If the curves were plotted with actual gradients instead of voltages, the experimental curve would follow more closely the probability curve. The experimental gradient curve would, however, for the smaller sizes bend up faster than the probability curve, due to greater apparent strength for smaller terminals, as for small spheres in the case of air. The curve between e/x and diameter for flat terminals of the larger sizes when the concentration at the edges is about constant should follow the probability curve. For example, suppose Fig. 156 represents a piece of solid insula- 176 DIELECTRIC PHENOMENA tion 0.025 mm. thick and sufficiently large to contain every condition of "weak spot." Divide this into six equal squares each of area a. The strength is marked on the various areas. Assume that an electrode is used giving no edge effect. With electrode of area a six tests are required to go over the whole piece. With electrodes of area 2a three tests are required, with area 3a two tests, and 6a one test. The following results may be obtained: Area No. of Total area Volts per mm electrode punctures covered Maximum Minimum Average a . . 6 6a 20 10 14 2a 3 6a 18 10 13 3a . . 2 6a 12 10 11 6a . 1 6a 10 10 10 The results are somewhat similar to the lower points of the curve in Fig. 155. On account of these characteristics alone an insulation built up of laminations is much better than a solid insulation as the weak spots in the laminations are not likely to line up. It is also much easier to make better and more uniform insulation in thin sheets. Another probable important reason for greater strength of laminated insulation is that the energy distances are interrupted by the discontinuous surfaces. Tests are useless for comparing insulation strengths unless made upon some standard basis. Great caution is necessary in the use of tabulated values of insulation strength in design. On account of the variable quality of solid insulation, tests must be continually made to see that the product does not change. Vacuum treatment is necessary before use to remove moisture. Even when all of the test conditions are known, experience is necessary to judge the proper factor of safety. Aside from this, stress concentrations due to the shapes and spacings of the con- ductors must always be considered and allowed for. It is gener- ally not possible to do this with mathematical exactitude, but approximation must be made with all factors in mind. Care must be taken that the solid insulation is below the rupturing gradient at any local point. If such a point is broken down locally the flux becomes still further concentrated. The puncture SOLID INSULATIONS 177 voltage will decrease with frequency, even over the commercial range, due to increasing loss with increasing frequency. Impulse Voltages and High Frequency. It takes energy and therefore time to rupture insulation. For a given potential a given number of cycles of very high frequency voltages, where heating does not result, are therefore much less injurious than the same number of cycles at low frequency. This also applies to impulse voltages of steep wave front. Continuously applied high frequency is, however, generally very injurious for two dis- tinct reasons: (1) On account of the very great loss at high frequency the insulation may be literally burned up in a very short time even at low voltages. This condition does not result in practice from surges, etc., on low frequency lines, but in high frequency genera- tors, and transformers, etc. In such apparatus it is important to use very smooth electrodes to prevent local concentration of stress and charring of insulation. This is especially so where contact is made with the air. If a local brush starts, on account of the great loss, it becomes very hot and extends out a consider- able distance. (2) In certain apparatus containing inductance and capacity very high local potential differences may be produced by reso- nance and thus cause rupture by overpotential. The high fre- quency thus does not cause the rupture directly but makes it possible by causing overpotential. Local concentration of stress may also result in non-homogeneous insulation, as across the condenser and resistance combinations in Fig. 152. The term "high frequency" is generally used in such a way that no distinction is made between sinusoidal high frequency from an alternator, undamped oscillations, damped oscillations, impulses of steep wave front, etc. Naturally the effect of con- tinuously applied undamped oscillations is quite different from a single high-voltage impulse of extremely short duration. As the effects are attributed to the same cause "high frequency" apparent discrepancies must result. (See comparative tests, Table LXXVI, page 184.) If the time of application is limited below a definite value, higher voltages are necessary to produce the same results in the limited time. Impulse voltages of steep wave front many times in excess of the rupturing voltage may be applied to insula- tions without rupture if the application is very short measured 178 DIELECTRIC PHENOMENA in microseconds. They may be caused in practice by lightning, switching, etc. If such voltages are sufficiently high, complete rupture may result at once. In any case if these voltages are higher than the 60-cycle puncture voltages the insulation will be damaged. As an example, an impulse voltage equal to three times the 60-cycle puncture voltage may be applied to a line insulator. During the very small time between the application of the voltage and the arc-over through the air, the insulator is under great stress. It may be that up to the ninth applica- tion of such a voltage there is no evidence of any injury, while on the tenth application failure results. Each stroke has con- tributed toward puncture. It is probable that each application adds to or extends local cracks. 1 Cumulative Effect of Overvoltages of Steep Wave Front. Voltages greatly in excess of the " rapidly applied 77 60-cycle puncture voltage may be applied to insulation without rupture if the time of application is sufficiently short. All such over- voltages injure the insulation, probably by mechanical tearing, and the effect is cumulative. A sufficient number will cause breakdown. For example: A piece of oiled pressboard 3.2 mm. thick has a rapidly applied breakdown at 60 cycles of 100 kv. maximum. If sinusoidal impulses reaching their maximum in 2.5 microseconds are applied, the number of impulses to cause break-down is as follows: Kv maximum of Number to cause impulse applied breakdown 100 140 100 150 s 16 155 2 165 1 If the impulses arc of still shorter duration, a greater number are required to cause breakdown at a given voltage. Insulations, and line insulators, are often injured and gradually destroyed in this way by lightning. Strength vs. Time of Application. It was stated above that the strength varies with the time of application, A curve is given in Fig. 153. The range of time shown in this curve is from a few seconds ("instantaneous") to an indefinitely long time. Over the greater part of the plotted curve heating is a factor and the great decrease is principally due to heating. Where the 1 See appendix. SOLID INSULATIONS 179 time of application is much less than " instantaneous " value, and heating can have no appreciable effect, the strength still increases very rapidly as the time of application is decreased. The increased strength at this part of the curve is due to limited energy, as explained on page 177. Some values from an actually measured curve are: (14 Layers Impregnated Paper between Concentric Cylinders) R = 0.67 cm. r = 0.365 cm. Kilovolts to puncture Time, sec. (maximum) 32 6 60 37 5 10 49 3 01 61 01 85 001 113 0.0001 196 / O- 5 \ g = 13 f 1 + 4 A) kv./mm max The equation of the strength-time curve over the complete range obtained from an examination of a number of curves is of the form a when T is the time of application in seconds, and g a is the gradient in kv./m.m. for indefinite time. The equation generally applies well over a range from infinite time to 0.01 seconds. For shorter periods many insulations shatter and fail at voltages lower than the equation indicates. Both a and g s vary with the thickness of the insulation, tem- perature, etc. In order that the strength may be high for indefinite time, the loss should be low. Permittivity of Insulating Material. In design, a knowledge of the permittivity of insulating materials is as important as the dielectric strength. For solid insulations the permittivity in- creases with the specific gravities of the material in almost a direct ratio. The various properties of some of the common insulations are given in Table LXXVL 180 DIELECTRIC PHENOMENA TABLE LXXVI. DIELECTRIC STRENGTH OF SOLID INSULATIONS Variation of Dielectric Strength with Thickness and Number of Layers. (One-minute Tests 60-cycle 10-cm Terminals in Oil. Values Effective Sine Wave) PRESSBOARD No of Thickness per Total thick- Kv /mm temperature 25 deg C layers layer, mm. ness, mm Varnished, Oiled transil, Linseed oil, kv./mm kv /mm kv /mm. 1 178 178 25 3 25 3 1 254 254 26 3 39 3 23 6 1 508 508 21 23 1 787 787 19 1 33 5 . 22 1 1 575 1 575 15 5 29 2 19 1 2 390 2 390 11 1 23 15.1 1 3 170 3 170 9 5 21 1 14 2 2 178 356 22 5 21 2 254 508 17 7 33 5 19 7 2 508 1 016 12 8 17 2 2 787 1 574 13 7 22 9 16 2 1 575 3 150 10 6 19,7 15 3 2 2.390 4 790 7 54 16.1 12 1 2 3 170 6 340 6 3 14 7 11 4 . 0.178 712 26 7 16 6 4 254 1 016 22 6 29 8 15 3 4 508 2.032 16 8 15 8 4 0.787 3.148 16 5 20 6 19 7 4 1 575 6 300 11 6 13 65 12.7 4 2 390 9.560 9 4 11 5 . 4 3 170 12.680 6.6 6 178 1 068 25 5 15 6 254 1 524 20 6 27 5 13 1 6 508 3 048 15.4 . . . . 14 4 6 787 4 702 14 9 20 17,8 6 1 575 9.450 11.3 TREATED WOOD Temperature 25 deg C. Across grain kv /mm. With grain kv./mm. 1 12 6 42 1 30 2.47 1 15 4 53 1 60 1 57 1 20 3 85 1 90 1 27 1 25 3 02 1 120 1.12 SOLID INSULATIONS 181 PAPER (Untreated) No of layers Thickness per layer, mm Total thickness, mm. 25 C., kv /mm 100C ,kv/mm. 1 064 064 9 3 9 3 1 127 127 8 7 7 9 1 254 254 7 9 7 3 4 064 258 8 7 8 3 4 127 508 7 5 6 7 4 254 1 016 6 6 6 2 8 0.064 516 8 7 8.1 8 127 1 016 7 4 6.6 3 254 2 032 6 3 6 VARNISHED CLOTH 1 305 30 26 2 23 6 2 305 61 20 5 19 7 3 305 91 18 5 17.0 4 305 1 22 16 8 14 9 5 305 1 52 15 5 13 1 6 305 1.83 14 6 11 5 7 305 2 13 14 10 3 8 305 2 44 13 3 9 2 9 305 * 2 74 12 8 8 3 10 305 3 05 12.3 7 5 HARD RUBBER No. of layers Thickness per layer, mm Total thickness, mm Puncture voltage 25 C>, kv /mm 100 C , kv /mm 1 0193 59 7 1 0.0223 55 6 1 0312 .... . 48.7 .... 1 2 2 17 3 1 3,0 3 14.2 1 4 4.0 12 7 1 5.0 5 11 8 .. 1 6 6.0 11.2 182 DIELECTRIC PHENOMENA MICA 1 0508 0508 96 5 1 0.1016 1016 88 7 1 1524 0.1524 75 5 1 0.2032 0.2032 62 6 .... 1 5080 0.5080 26 1 Total thickness 6 GLASS Kv./mm. 10 The kv./mm. strength of glass decreases rapidly with increasing thickness. PORCELAIN Total thickness, mm. Kv /mm 5 16 1 14.5 2 12.2 5.0 11 10.0 9.6 15 9 2 VAEIATION OP INSULATION STRENGTH WITH TIME OF APPLIED VOLTAGE Material Thickness, mm. Time to puncture, mm 25 C kv /mm. 100 C kv /mm. Oil impregnated paper, 1,90 "Inst." 39.4 32 30 layers, 60-cy., 10- 1 33.1 27.3 em. diameter discs, 2 31.0 25.7 round edges. 4 29 2 24.5 6 28 2 23 6 10 26.8 22.7 20 25 5 21.6 40 23.6 20.5 60 22.7 19.7 80 22.1 19 3 100 21 6 19.0 Note that for a given thickness the strengths of materials do not vary as greatly as might be expected. SOLID INSULATIONS 183 Material Thickness, mm Time to puncture, mm Puncture voltage, 25 C 1 layer, 0.30 mm kv /mm 5 layers, 1.50 mm kv/mm 10 layers, 3 mm kv /mm Varnished cloth, 30 mm., 60-cy., 10-cm. diameter in air, round edges 30 "Inst." 1 2 5 1 2 3 5 10 20 52 5 37 7 34 5 32 8 32 5 32 1 31 8 31 5 31 1 30 2 36 1 27 5 25 8 22 9 21 20 3 19 9 19 8 19 7 19 6 27 2 22 3 19 7 16 4 14 3 13 12 6 12 5 12 3 9 9 PERMITTIVITY OF INSULATING MATEKIALS Permittivity Specific gravity to Asphalt . . . Bakelite. . . Cambric (varnished) . Fiber (horn) dry Fiber (horn) oil. . . 4-^ to 5 Glass (crown) 6 Glass (heavy flint) 10 Gutta percha Lead stearate 5.2 Lead palnritate 5.2 Lead oleate 5 Mica 5 to 7 Oil (linseed) OiJ (transil) 2 to Paper (dry) 26 Paper (paraffined) Paper (oiled) 4 Paraffme 2 to 2.3 1 15 7 to 1 0.9 to 1 5 3 to 3. 5 4 5 0,95 O.StoO 9 1.00 1.25 0.9 184 DIELECTRIC PHENOMENA PERMITTIVITY OF INSULATING MATERIALS Continued Permittivity Specific gravity Pressboard (dry) Pressboard (oiled) Porcelain 3 4 to 6 4~j4 to 5 1 25 1 40 2 4 Rubber (hard) Rubber (vulcanized) 3 2-H Shellac Sulphur 3 4 Wood (treated) 3 to 3-# 8 to 9 COMPARATIVE INSULATION STRENGTH FOR HIGH FREQUENCY, IMPULSE, OSCILLATION AND 60-CYCLE VOLTAGES Temperature 30 deg C 60 Cycles High frequency (alternator), 90,000 cycles Damped oscilla- tion, tram freq 120 sec., 200,000 cycles Single impulse, sine shape, cor- responding to half cycle of 200,000 cycle Thickness, mm ! Inst. 1 mm. Inst. 1 min. Inst. 1 min. kv /mm. (max.) kv./mm. (max ) kv./mm. (max.) kv./mm, (max.) Transil Oil between Flat Terminals Square Edge 2 5-cm. Diameter, 0.25-cm. Space 17 6 7 30 39 Oiled Pressboard 10-cm Diameter Square-edge Discs in Oil 35 5 31 9 5 7.3 37 V 29.0 72.0 2.5 I 39 5 37 6 1 4 1 42 24.0 5 2 2,5 1 76 15 3 Varnished Cambric 53,0 46 5 19 5 17 6 108 6 ?, 42 31 13 5 10 55 56 78 1.5 5 37 28.0 10.0 7.3 49 41 70.0 2 5 8 33.0 27 5 41 30 5 60 3.6 12 SOLID INSULATIONS 185 Energy Loss in Solid Insulation. In general, energy loss in solid insulation: (1) Increases with increasing voltage. (2) Increases with increasing temperature. (3) Increases with increasing frequency (4) Increases with increasing moisture content. (5) Increases with increasing impurities, as occluded air, etc. .28 .24 .22^ *y .08 20 .06 .04 10 .02 1.1 ___ FIG. 157. Insulation loss and power factor at 60 ~. (Oiled'pressboard 5 mm. thick between parallel plates with rounded edges in oil. Curves 1, 2, 3, 4, watts per cu. cm. Curves 5, 6, 7, 8, Power factor ) r 20 20 IS 18 16S16 g,1212 |.08|8.0 .00 8.0 .02 2,0 30 40 50 60 70 Temperature-Degrees Cent. FIG. 158. Insulation loss and power factor vs. temperature at 60 ~. (Data, Fig. 157.) For good uniform insulation free from foreign material, mois- ture, etc., the loss at constant temperature and frequency varies approximately as the square of the applied voltage. The author has found that approximately for good insulations p = a/e 2 = bfg* X 1CT 6 watts/cu. cm. t 186 DIELECTRIC PHENOMENA where/ frequency in cycles per sec. g = gradient kv./mm. effective. b = constant varies with different insulations. It is 8 to 10 for varnished cambric in a uniform field, and thickness in order of 5 mm. (25 C.). Compare calculated values with values given in Table LXXVII at both 60 cycles and high frequency (25 deg. C.). With occluded air or water, where the Pr loss becomes large in comparison with the " hysteresis" loss, the rate of increase is greater. Due to combinations of resistance and capacity it may then take the form, 1 p = fc/g 2 + (c/y + ag*). Fig. 157 shows characteristic curves between energy loss, power factor, and voltage of insula- tion in good condition. The loss increases very rapidly with temperature. The tem- perature curves are shown in Fig. 158. The effect of exposing to the air is also shown. Loss in different insulations is given in Table LXXVII. TABLE LXXVII. INSULATION LOSSES (Effective Sine Wave 60 Cycles) Total thickness, mm Insulation No of layers Temp , deg C Volts per mm. Watts per ou cm 4 Varnished cloth. 15 25 4,000 005 6,000 015 8,000 035 10,000 0.060 12,000 090 4.0 Varnished cloth 15 90 4,000 0.025 6,000 075 8,000 150 10,000 0.240 12,000 0.350 2 5 Oil-treated paper 30 25 10,000 0.040 14,000 070 2 5 Oil-treated paper 30 60 10,000 0.043 14,000 080 2.5 Oil-treated paper 30 90 10,000 050 14,000 100 2 5 Oil- treated paper 30 120 10,000 0.067 14,000 0.138 These losses may be lower or very much higher, depending upon the con- dition of the insulation. 1 See Fig. i52. SOLID INSULATIONS 187 HIGH FKEQUENCY Loss IN DIFFERENT INSULATIONS (Alexanderson, Proc. Inst. Radio Engrs , June, 1914) Volts per mm Effective Frequencj* kilocycle Material (thickness 5 mm ) Glass Mica Varnished cambric Asbestos Loss watts, cu cm. P F. avg Loss watts, cu cm. P F. avg. Loss watts, cu. cm P. F. avg Loss watts, cu cm P F. avg 500 20 02 02 7 500 40 05 1 4 04 1 8 08 ." 1 3 500 60 08 05 12 3 3 2 500 80 11 08 18 32 1000 20 08 07 3 1000 40 20 1 4 12 1 8 28 5 3 1000 60 32 24 . 45 3 3 7 6 32 1000 80 40 0,35 65 The rate of increase of the loss with the frequency will vary greatly if the insulation contains moisture. If the moisture is arranged in such a way as to approximate a condenser and resist- r I | / n \J\ s W-" ,--* -*" \ 1 50 100 JKilovolts-High Tension FIG. 159 Dielectric loss vs. voltage in a 2750 kv-a, 120 kv, 60- transiormer. o 10 20 o so Temperature Else above 21 0. FIG 160. Dielectric loss vs. tem- perature in a 3750 kv-a, 120 kv. 60 transformer at 100 kv ance in series, as in Fig. 152, the loss may, over a limited range, increase approximately as the square of the frequency. If the insulation is in good condition the loss may increase approxi- mately directly as the frequency. The best method of comparing different insulations is by meas- urement of losses. Operating Temperatures of Insulations. The maximum operating temperature of insulations is indefinite. For low-vol- 188 DIELECTRIC PHENOMENA tage apparatus, temperatures not high enough to cause direct electrical failure may cause mechanical failure m short periods by drying out the insulation, cracking, etc. The maximum safe temperature, at which the life is not greatly shortened mechan- ically by cracking, drying out, etc., varies with different insula- tions, but is approximately as follows : Fibrous materials, cloth, varnish, etc 100 deg C Asbestos, mica and similar materials, in combination with binders' varnish, etc . .150 deg C. Mica, asbestos alone . . very high. These valufes are given without consideration of the electrical effects. Often the electrical properties will limit the tempera- tures below these values. Heat conductivity must be considered in design. 140 130 120 345 Total Arcing Distance -^ FIG 161. Surface arc-over in oil. (Hendncks ) Surface Leakage. Strictly speaking, on clean dielectric sur- faces, appreciable leakage does not occur. What is generally termed " surface leakage " is a rupture of one dielectric at the surface of another dielectric by o verflux concentration due to differ- ence in permittivities, etc. For instance, on a porcelain insulator in air the flux may be sufficiently concentrated at portions of the surface to cause the air to rupture. The appearance is that of leakage over the porcelain surface. " Surface leakage 7 ' then is quite indefinite, and for a given leakage distance depends upon the position and shape of the electrodes, relative capacities of the materials, etc, (See Fig. 161.) The effects of actual leakage and SOLID INSULATIONS 189 apparent leakage in air may be seen in Table LXXVIII, page 190. In (1) the spark-over is given with the surface out. In (4) the decrease must be due to actual leakage as there is no flux concentration. In (2) and (3) flux concentration is balanced against increased surface. Solid Insulation Barriers IB. Oil. Properly placed barriers of solid insulation in oil greatly increase the strength of the oil spaces by limiting the thickness of the oil, preventing moisture chains lining up, etc. This should always be considered in design. In placing barriers, however, the arrangement should be such that the stress on the oil is not increased by the higher permit- tivity of the solid insulation. Data for a simple arrangement are given in Table LXXVIII. It will be noted that in most cases the strength is not greatly increased on account of difference of per- mittivity of oil and solid insulation. The reliability is much greater, however. TABLE LXXVIII. PRESSBOARD BARRIEES IN OIL Gap 24 cm. Oil only. . 1 08-cm sheet of pressboard midway between electrodes . 1 08-cm. sheet of pressboard against one electrode . ^ Kv effective 23 24 7 22 7 Gap 0.40 cm. Oil only ... . ... ... 2 0.08-cm. sheets of pressboard against one electrode. . Kv effective 35 3 36 5 Gap 0.56 cm. Oil only 3 08-cm sheets of pressboard against one electrode. Kv. effective 53.9 44 Kv. Gap 1 16 cm. effective Oil only. 960 1 0.08-cm sheet of pressboard 0.1 cm. from each terminal . 95 3 1 08-cm. sheet of pressboard 33 cm. from each terminal 102 2 08-cm. sheet of pressboard at midpoint. 88 5 1 0.08-cm sheet of pressboard on each terminal 94 5 Strength of pressboard 08 cm., 15 kv ; 16 cm , 28 kv. Terminals 6 cm. in diameter, rounded with a 3-cm. radius at, the edges. 190 DIELECTRIC PHENOMENA SURFACE ARC-OVER IN Am 1 (1) 7.6 cm. Air only between plates. Rounded edges Effective kv. kv./cm. parallel 128 16 8 y* (2) 7.6 cm. Over corrugated rubber cylin- der between above plates. Surface oiled Surface dry 94 87.0 12 4 11 4 (3) Corrugated rubber cylinder between above plates. Surface oiled 109 14 3 Surface dry 89.0 11.7 t (4) Smooth rubber cylinder between above 7.6 cm* plates. Oiled surface 122.0 16.0 Surface dry 62.0 8 \ NOTE. Maximum possible kv. arc-over 128. Data shows that although corrugations increase stress, actual gain is made by their use by reduction of true leakage. Impregnation. Insulations, such as dry paper, with low dielec- tric strength and low permittivity, are impregnated with oils or compounds of high strength and permittivity. The result is a dielectric of greater strength and permittivity. If the impreg- nating is improperly done, for instance so as to leave oiled spots and unoiled spots, the dielectric strength may be less than the dry paper alone. This is due to the difference in permittivities of the dry and oiled spots, which causes a concentration of stress on the electrically weak' dry spots. Mechanical. It is of great importance to arrange designs in such a way that local cracking, or tearing, is not caused by high localized mechanical stresses. This is especially so with porce- SOLID INSULATIONS 191 lain, as in the line insulators. Expansion of a metal pin, localized mechanical stress due to sharp corners, expansion of improper cement, etc., will cause gradual cracking of the porcelain. The so-called deterioration of line insulators is often caused in this way. Direct Current. As the breakdown depends upon the maxi- mum point of the voltage wave, the direct-current puncture vol- tage in air and oil is (\/2) or 1.41 times the sine wave alternating puncture voltage. In air and oil there is very little loss with alternating current until the puncture voltage is reached. With solid insulation losses occur with alternating current as soon as voltage is applied. In the time tests the insulation is thus considerably weakened by heating, especially thick insulation. This causes decreasing breakdown voltages in the time tests as the frequency is increased. In certain insulations the loss is very small for direct current. The gain for direct current in solid insulation in the time tests is thus greater than the 41% given above. See appendix. Occluded Air. Where careful work is not done air films may be occluded in solid insulations. Such films are likely to break down and cause local heating, chemical action and finally, breakdown of the solid insulation. When such films are un- avoidable, the stress should be limited below the breakdown of air. The strength of such film is the same as between metal electrodes. See data appendix. CHAPTER VIII THE ELECTRON THEORY A brief review of the electron theory will be given in this chapter. A gas is a very poor conductor of electricity. A condenser or electroscope may be left charged in air a great length of time with- out considerable loss or leakage. If, however, the surrounding air and the terminals of the condenser or electroscope are sub- jected to the action of X-rays, ultraviolet light, or radio-active substances, the leakage becomes quite rapid. All of these agents in some way act as carriers or change the nature of the gas so that the current passes from terminal to terminal. The gas is said to be ionized. FIG. 162 Cathode ray tube. If terminals are placed in a vacuum tube and high voltage is applied between them, a visible discharge or beam of rays is shot out from the cathode. These cathode rays proceed in straight lines. A pin-hole diaphragm may be placed in their path and a narrow beam obtained (see Fig. 162). This beam may be de- flected by a magnetic or dielectric field. J. J. Thomson pointed out that it acts in every way as if it were made up of negatively charged particles traveling at very high velocities. 1 Every test that has been made bears this out. Where the particles strike the glass it becomes luminescent. These particles of negative electricity or "charged" corpuscles are called electrons. The velocity, "charge," and mass of these electrons have been measured. 1 These rays have been made use of in an oscillograph In this instrument the beam acts as a pointer and is made to trace a curve under influence of the fields produced by the current or voltage of the wave which is being measured. 192 THE ELECTRON THEORY 193 A "charged' 7 body in motion is deflected by the electric fields in the same way as a wire-carrying current. The deflection de- pends upon the ratio of the " charge 77 e and the mass m. By noting the deflection of the cathode rays in the electric field, J. J. Thomson found the value of the ratio e/m. The most accurate value of the ratio with e measured in electromagnetic units is 1.8 X 10 7 . Each ion in a gas acts as nuclei in the condensation of water vapor. The condensation in the presence of the ions may be made to occur by change of pressure. By observing the rate of fall of the cloud the number of drops or electrons can be calculated. If the total " charge 77 is measured, e can be at once obtained. This was done by C. T. R. Wilson, e was also later determined by Millikan and found to be 4.77 X 10- 10 electrostatic units or 1.6 X 10~ 20 electromagnetic units. The mass of the electron seems to be about 1/1800 of the hydrogen atom, or the same mass as the hydrogen ion in electrolytic conduction. This mass is about 8.9 X 10- 28 grams when the velocity is considerably below that of light, and apparently changes with velocity. It must be considered as that determined by force divided by acceleration. The velocity of the electron varies from 10 7 to 10 9 cm./sec. The beta particle of radio-active substances is identical with the cathode particle or electron. The gamma rays are, probably, ether waves produced by the action of the beta particles in a way similar to that in which X-rays are produced by the im- pingement of cathode particles on solids. The alpha particle is a positively charged atom of helium. Elemental positive particles corresponding to the electron have so far not been found. Ion is a general term used for positive or negative atoms or molecules, electrons, or positive particles. Take two electrodes in air and apply some low potential between them. Direct ultraviolet light upon the negative electrode. If the voltage is gradually increased, the current in- creases almost directly up to (a), Fig. 163. There is then a con- siderable range between (a) and (b) where an increase in voltage does not greatly increase the current. At (b) the current sud- denly increases very rapidly with increasing voltage. It appears that negative " particles 77 or electrons are produced or set free at the negative conductor by the ultraviolet light. These "particles of electricity 77 are attracted to the positive conductor and thus show as current in the galvanometer in the circuit. The number reaching the positive conductor increases with in- 194 DIELECTRIC PHENOMENA creasing voltage. The current thus increases with increasing voltage. The potential at (a) is sufficient to cause practically all of the negative particles that are produced by the light to reach the positive conductor. An increase of the voltage above the value at (a) can thus cause very little increase in current unless a new source of ionization is applied or the number of ions is increased in some way. When the voltage is raised above the value at (&), the current increases very rapidly with increasing voltage. A new source of ionization has resulted. The velocity at which ions travel increases with increasing voltage or field intensity. The new source of ionization results when the ions have reached a definite velocity in their mean free path. Townsend has ex- plained this on the hypothesis that ions traveling at suffi- cient speed generate new ions on collision with neutral atoms or molecules. Thus after a sufficient voltage is applied, the velocity of the ions in their mean free path becomes great enough to pro- ~~~fe FIG. 163. Variation of current with voltage through ionized space between parallel plate electrodes duce new ions by collision with atoms or molecules by separat- ing the positive and negative These in turn produce new parts of the atoms or molecules, ions so the ionic density increases very rapidly. The positive ions travel to the negative conductor; the negative ions to the positive conductor. It seems, however, that the electron plays the principal part in impact ionization. It may be of interest to review in a brief way how the law of visual corona was derived, to show that it is a rational law, and to illustrate a practical application of the electron theory. In 1910 an investigation was conducted in which the visual corona voltages of various sizes of polished parallel wires at various spacings were determined. 1 For any given conductor the voltage gradient at rupture, g v , was found to be constant independent of the spacing (except at very small spacings), but increased very rapidly as the radius of the conductor was decreased. Thus air apparently had a greater strength for small conductors than large 1 F. W, Peek, Jr., Law of Corona, A.I.E.E., June, THE ELECTRON THEORY 195 ones. This was formerly pointed out by Prof. Ryan. The curve of experimental data between g v and radius r was found to be regular and continuous. A number of equations could readily be written which would fit these data. It was desired, however, to establish or build up a rational equation. The old idea of air films at the surface of the conductors was abandoned after tests with very light (aluminum) and very heavy (tungsten) metals showed that the density of the metal of the conductor had no influence on g V9 which should be the case if the difference were caused by air films, as the air film should vary with the density of the conductor. A rational law of visual corona was deduced from the data, as follows : Energy of some form, be this the ^. -5- of the energy of the moving ions, or whatever form it may, is necessary to rupture insulation. This is borne out by experiments with transients, which show that finite time is necessary to rupture insulation; that if this time be limited the voltage must be increased to accomplish the same results in the limited time, also heating results at rupture, etc. These imply definite finite energy. The gradient or stress to rupture air in bulk in a uniform field, g , should be constant for a given air density or molecular spacing. In a non-uniform field, as that around a wire, the breakdown strength of air, g 0) is first reached at the conductor surface; at an infinitely small distance from the conductor surface the stress is still below the rupturing gradient. Hence, in order to store the necessary finite rupturing energy the gradient at the conductor surface must be increased to g v , so that at a finite distance away the gradient is g . This means that a finite thickness of the insulation must be under a stress of at least g . The ruptur- ing energy is in the zone between g v and g > The thickness of the zone should be a function of the conductor radius. It was found that at cm. from the conductor surface the gradient at rupture is always con- stant and 30 kv./cm. (at standard air density). The relation between g v and r may now be directly expressed by the simple law = g /, , 0.301\ OA / 1 , 0.301A , , , , 1 H -- T=- = 30 1 H -- 7=- kv./cm. (max.) \ V r I \ V r I 196 DIELECTRIC PHENOMENA For parallel planes or for air in bulk 7* = oo ffv 9o Thus the strength of air is constant and equal to 30 kv./cm., but in non-uniform fields is apparently stronger, as explained above. If the air is made less dense, that is the molecular spac- ing is changed, the strength of air in a uniform field should de- crease directly with the air density. g'o = 8g However, for non-uniform fields, the energy distance should also change thus The complete equation including air density factor was found to take the simple rational form This equation holds for values of 8 as low as 0.02 for corona on wires. For a given pair of electrodes the strength, g, decreases with decreasing 8 until a minimum value is reached. g then increase's very rapidly with decreasing 8. See Fig. 164. The value of 8 at which the minimum g occurs in a uniform field, as between spheres at small spacings, x, depends upon the product FIG. 164. Variation of strength of of x and pressure, #, or of X air with density showing increase in j mi , strength at very low densities. ancl 5 * JL*n$ means that the spark potential is constant as long as the product of the pressure or density and spark lengtli remain constant, 'Thus where or px = k 8x = the spark-over voltage is constant independent of the individual values of p and x. See appendix. This is known as Paschen's Law, At very high vacuum the separation of the molecules THE ELECTRON THEORY 197 may be of a fairly high order compared to the dimension of the tube. There is, thus, very little ionization by collision, and the apparent strength becomes high. At still higher vacuum, as used in the best X-ray tubes, the only source of ionization is from the conductors themselves. In the latest tubes the cathode is hot and is the only source of ions. The number can be con- trolled by the temperature of the cathode. 1 If the energy distance is limited to less than0.301\/r, by placing the conductors close together, the apparent gradient should in- crease. This also is borne out by experiment. The visual tests on various forms of electrodes, as spheres, wires, planes, etc., as well as loss measurements, all point to an energy storage distance and a constant strength of air of 30 kv./cm. For continuously applied high frequency where the rate of energy or power is great, frequency may enter into the energy thus, 0.301^ (/) and spark-over take place at somewhat lower voltages. Where the time is limited, as by an impulse of steep wave front, a much higher voltage should be required to start arc-over. This is also borne out by experiment. Thus far the form of this rupturing energy has not been con- sidered as it was unnecessary, in order to develop a rational working equation. When low potential is applied between two conductors any free ions are set in motion. As the potential and, therefore, the field intensity pr gradient is increased, the velocity of the ions increases. 2 At the gradient of g = 30 kv./cm. (5 = 1) the velocity of the ions becomes sufficiently great over the mean free path to form other ions by collision. This gradient is constant and is called the dielectric strength of air. When ionic saturation is reached at any point, the air becomes conducting and glows, or there is corona or spark. Applying this to parallel wires: when a gradient g v is reached at the wire surface, any free ions are accelerated and produce other ions by collision with molecules, which are in turn acceler- ated. The ionic density is thus gradually increased by successive collision until at 0.301V? cm. from the wire surface, where g = 30, ionic saturation is reached, or corona starts. The distance 1 Coolidge X-ray tube. 2 See also explanation given in Theory of Corona, Bergen Davis, A.I.E.EL, April, 1914. 198 DIELECTRIC PHENOMENA 0.301 Vr cm. is, of course, many times greater than the mean free path of the ion, and many collisions must take place in this distance. Thus, for the wire, corona cannot form when the gradient of g is reached at the surface, as at any distance from the surface the gradient is less than g . The gradient at the surface must therefore be increased to g v so that the gradient a finite distance away from the surface (0.301 \/r cm.) is g . That is to say, energy is necessary to start corona, as noted above. g the strength of air, should vary with 5; g v , however, cannot vary directly with <5, because, with the greater mean free path of the ion at lower air densities, a greater "accelerating" or energy distance is necessary. In the equation, a = 0.301 Vr/^; that is, a increases with decreasing 5. When the conductors are placed so close together that the free accelerating or energy storage distance is interfered with, the gradient g v must be increased in order that ionic saturation may be reached in this limited distance. Over a wide range, initial ionization of the air cannot affect the starting voltage of a steadily applied low-frequency e.m.f. since such ionization must necessarily be very small compared to the residual ionization after each cycle. If the ionization is very small when such a voltage is first applied an appreciable time is necessary before corona starts, but the starting voltage is not affected. The initial ionization should, however, have a considerable effect upon transient voltages of short duration, steep wave-front voltages, etc. Thus, if for given electrodes, the time of applica- tion is less than that normally necessary to bring the initial ioniza- tion up to ionic saturation, a higher voltage should be required to cause corona or spark-over in the limited time. Experiments show, however, that even with impulse voltages the initial ioniza- tion may be varied over a great range without appreciable change in the impulse spark-over voltage of a given pair of electrodes in open air. The effect of initial ionization may be observed to a greater extent at low air densities, where the number of free ions may be made an appreciable per cent, of ionic saturation. When the electrodes are of such a nature as to require considerable brush discharge in the path of the spark before spark-over, the steep wave-front voltage required to cause discharge over a given gap is much higher than the required steady voltage. If spheres and needles, set to spark-over at the same 60-cycle voltage, are placed in parallel and impulse voltage of steep wave front ap- plied, spark-over will take place across the spheres only. CHAPTER IX PRACTICAL CORONA CALCULATIONS FOR TRANSMISSION LINES Summary of Various Factors Affecting Corona. If potential is applied between the conductors of a transmission line and gradu- ally increased, a point is reached when wattmeters placed in the circuit begin to read. The watt loss is low at first but increases with increasing voltages. At the point where the meters begin to read, a hissing noise is heard, and if it is quite dark, localized 16 .30 15 .28 14 .26 13 .24 12 g.22.11 1 .20 JlO S -18 | 9 | ,16 S 8 B, .12 6 * .10 B .08 4 .06 3 .04 2 .02 1 n 1, I 1 i f. A & S V i <$ X S* // \> s S 7 */ X * V* / ^ ^x / J w in 10 / ta Q I ? e 1 o o bo d i? 1 "s / B / 4 o 1 9 S / V t ;y o 5 4c J? P c r H > c 3 S M H 5 S ii 2 S i r \\ \ | \ I ii Effective Kilo-Volts Between Lines Effective Kilo Volts Between, Lmes FIG. 166. Characteristic corona loss, FIG. 167. Loss near the critical current, and power factor curves. voltage of new and old cables. (Line A. Conductor length, 109,500 (Data Fig. 166. Line calcu- cm. (total). Spacing, 3 10 cm Diameter, lated. x, new cable, o, weathered 1.18 cm. (3/0 cable). Temp., 12 C. cable). Bar , 75.) streamers and glow points can- be noticed at spots on the con- ductors. These first streamers are caused by dirt and irregulari- ties. The watt increase is still gradual. Slowly raising the voltage, the true visual critical corona point is finally reached. The effect is striking; corona suddenly jumps out, as it were, all along the line. The line immediately becomes very noisy, and the loss increases very rapidly with increasing voltage. The intensity of the light also increases with increasing voltage. If 199 200 DIELECTRIC PHENOMENA one is close to the conductors an odor of ozone and nitrous oxide, the result of chemical action on the air, is noticed. There is, thus, heat, chemical action, light, and sound in the process of corona formation. These naturally all mean energy loss. It becomes of great importance in the design of high-voltage transmission lines to know the various factors which affect the corona formation, and to have simple working formulae for pre- determining the corona characteristics, so that the corona loss will not be excessive. Loss begins at some critical voltage, which depends upon the size and spacing of the line conductors, altitudes, etc., and in- creases very rapidly above this voltage. Figs. 166 and 167 show typical corona loss curves during fair weather. An extensive investigation on an experimental transmission line (see Fig. 168) has shown that the corona loss in fair weather is expressed by the equation : p = a(/+ c)(e - 6 ) 2 where p = loss in kilowatts per kilometer length of single-line conductor. e = effective value of the voltage between the line con- ductors and neutral in kilovolts. 1 / = frequency. c = a constant = 25 and a is given by the equation A a = - where r = radius of conductor in centimeters. s the distance between conductor *and return con- ductor in centimeters. 5 density of the air, referred to the density at 25 deg. C. and 76 cm. barometer as unity. A = a constant = 241. e = the effective disruptive critical voltage to neutral, and is given by the equation e = m goSr log, s/r kv. to neutral 1 where g is the disruptive gradient of air in kilovolts per centi- meter at 25 deg. C. and 76 cm. barometer, and is constant for all 1 Hence, in single-phase circuits, e is one-half the voltage between con- ductors. In three-phase circuits, e is l/\/3 times the voltage between conductors. ^^^^^""""^^ii^^MMMH^^^^^^^^^^BlalllBlBMilHI Corona at 230 kv. Line A. 3/0 cable. 310 cm. (122 in.) spacing (Pacing page 200. FIG. 168. Experimental transmission line. CORONA CALCULATIONS FOR TRANSMISSION LINES 201 practical transmission line sizes of conductor frequencies, etc. For very small conductors q& is used. (See pages 136, 141, 142.) g = 21.1 kv. per cm. (effective). m is a constant depending upon the surface condition of the conductions, and is m 1 for perfectly smooth polished wire, m = 0.98 to 0.93 for roughened or weathered wires, and decreases to m = 0.87 to 0.83 for seven-strand cables (where the radius is taken as the outer radius of the cable) . Luminosity of the air surrounding the line conductors does not begin at the disruptive critical voltage e ot but at a higher voltage e v , the visual critical voltage. The visual critical voltage, e v , is much higher for small conductors than the disruptive critical voltage, e ; it is also higher for large conductors, but to a less extent. For very small conductors e d replaces e . (See page 141.) While theoretically no appreciable loss of power should occur below the visual voltage, e v , some loss does occur, due to irregu- larities of the wire surface, dirt, etc., as indicated by brush dis- charges, and local corona streamers. (See page 143.) As the loss between e v and e depends upon dirt, roughened condition of the wire surface, etc., it is unstable and variable and changes as the surface of the conductors changes. For the larger sizes of stranded transmission conductors in practice the surface is generally such that the loss approximately follows the quadratic law, even between e and e v . This is shown by the circles in Fig. 167, which are measured points on a weathered conductor. The crosses indicate how the points come on a new conductor. For a small conductor the difference between the calculated and measured losses on the section of the curve between e and e v is still greater. Above e v the curves coincide and follow the quadratic law. In practice it is rarely admissible to operate above the e voltage. 1 Cases are known in which conductors have deteriorated by the action of nitric acid formed by exces- sive brush discharge. It is interesting to note that the loss below e v actually follows the probability curve but this need not be considered in practice. 1 Operation at e voltage at high altitudes gives relatively greater margin and less loss than at sea level as there is greater difference between e v and e . 202 DIELECTRIC PHENOMENA 7m. The corona loss is: (a) A loss proportional to the frequency / plus a small constant loss. (&) Proportional to the square of the excess voltage above the disruptive critical voltage, e . (c) Proportional to the conductor radius r and log s/r. The critical voltage thus increases very rapidly with increasing r, and to a less extent with spacing. The disruptive critical voltage, e , is the voltage at which the disruptive voltage gradient of the air is reached at the conductor surface. Hence it is: (a) Proportional to the conductor radius r and log e s/r. The critical voltage thus increases very rapidly with increasing r, and to a much less extent with increasing s. (6) Proportional to the air density or becomes very low at high altitudes. (c) Dependent somewhat on the conditions of the conductor surface, as represented by m. The effects of various atmos- pheric conditions and storms on the critical voltage and loss will now be considered. (a) Humidity has no effect on the critical voltage. Fio. 169.-Compar.son of fair ^ Smoke . lowers the f 1 tical weather and storm loss, voltage and increases the loss. (c) Heavy winds have no effect on the loss or critical voltage at ordinary commercial frequencies. (d) Fog lowers the critical voltage and increases the loss. (e) Sleet on the wires, or falling sleet, lowers the critical voltage and increases the loss. High voltages do not eliminate sleet formation. (/) Rain storms lower the critical voltage and increase the loss. (g) Snow storms lower the critical voltage and increase the loss. (h) At high altitudes the loss is very much greater on a given conductor, at a given voltage, than it is at sea level. For a given voltage larger conductors must be used at high altitudes. 18 17j 16 15 14 13 12 211 I 9 8 8 S Kilo-Volts Effective CORONA CALCULATIONS FOR TRANSMISSION LINES 203 Fig. 169 shows a typical loss curve during storm and a corre- sponding fair weather curve. Practical Corona Formulae and Their Application. The for- mula required for the determination of the corona characteristics of transmission lines are: METRIC UNITS Disruptive Critical Voltage e = 21.1m rdloge s/r kv. to neutral (35) Power Loss Where the conductors are small use formulae (34a), (35a), and (36), Chapter V. Visual Critical Voltage e v = 21.1m v 8r(l -\ -- =- ) log e s/r kv. to neutral (20) V V5r/ 3926 o = 273 + t where e = effective kilo volts to neutral applied to the line 1 5 = air density factor = 1 at 25 deg. C., 76 cm. barometer 6 = barometric pressure in centimeters t = temperature in degrees Centigrade r = radius of conductor, centimeters s = spacing between conductor centers in centimeters / = frequency cycles per second. For approximating storm loss consider e = 0.8 of fair weather value in formula (35). Irregularity Factors m = 1 for polished wires = 0.98 0.93 for roughened or weathered wires = 0.87 0.83 for seven-strand cables m v = m for polished wire 1 m = 0.72 for local corona all along cable m v *= 0.82 for decided corona all along cable. 1 e =s volts between line times l/\/3 for three-phase lines and volts between line times H for single-phase or two-phase lines. 204 DIELECTRIC PHENOMENA ENGLISH UNITS Disruptive Critical Voltage e = 123m rd logio s/r kv. to neutral Power Loss kw. of single conductor p , _ , N (/ + 25)Vr/s(e - )l e / 1 A V '^ 34 oo \ 30 9 ( yd 8 28 y 26 / / 04 / L cy lea Kilo-Watts jjer Mile of Li |_l M M I-* H* tO tO t 5 tO #>. Cl 00 O tO l" O> 00 O N ll 1 1 / I 1 J r 1 /I r / e 'v / / / 1 / ' X / '/ 130 KKoctive Kilo-Volts Between Lines 40 50 60 70 8090100110120130140 Effective Kilo-Volts FIG. 173. FIG. 174. Comparison of calculated and measured losses. FIG. 173. Leadville. Three phase. (Test made by Faccioli ) 1/0 weathered cable. Spacing (flat) 124" (3 14cm ). Diam-eter, 95cm Length of line, 63.5 miles (one conductor). Temp., 11 C Bar., 60 cm. Frequency, 60. Curve calculated, x measured. FIG. 174 Outdoor experimental line. (Tests by A B Hendricks, Pitts- field, 1906.) Wire conductor. Diameter, 064" (radius 081 cm.). Spacing, 48" (132 cm ). Length, about 800 ft. 5=0 97. applied in the predetermination of the corona loss of commercial transmission lines. 2 The Corona Limit of High-voltage Transmission, with Tables. The question is often asked, what is the limiting distance im- 1 N. E. L. A., June, 1912 2 Peek, F. W., Jr Comparison of Calculated and Measured Corona Loss, A. I. E. E., Feb., 1915. 210 DIELECTRIC PHENOMENA posed on high-voltage transmission by the corona limit of vol- tage? In the first place it does not seem at present, except in very rare instances, that corona will be the limiting feature at all. The limiting feature will, in all probability, be an economic one; the energy concentrated naturally at any given point will be exceeded by the demand in the surrounding country before the transmission distance becomes so great that voltages above the corona limit are necessary. A quarter of a million volts may be used (except at high altitude) without an excessive conductor diameter or spacing (See Tables LXXX, LXXXI and LXXXII.) * TABLE LXXX CORONA LIMIT OF VOLTAGE 2 Stranded Cables Kilovolts between Line Three-phase Sea Level and 25 deg C Size B & S or cir mils Diameter, inches Spacing, feet 3 4 5 G 8 10 12 14 16 20 4 230 56 58 60 62 64 66 68 69 71 3 261 62 65 67 70 72 74 76 77 80 2 290 71 73 76 79 81 83 85 87 1 330 79 81 85 88 91 93 95 97 374 90 95 98 102 104 108 109 00 420 98 104 108 111 114 117 121 000 470 114 118 121 124 127 132 0000 530 125 130 135 138 141 146 250,000 300,000 590 620 138 144 151 149 156 152 161 156 165 161 171 350,000 679 161 166 170 175 180 400,000 450,000 500,000 728 770 818 171 178 188 176 184 194 180 190 199 185 194 205 192 200 210 800,000 1,000,000 1.034 1 152 234 256 241 264 244 270 256 281 1 These tables will give an approximate idea of the voltage limit imposed by corona. In general it will be found advisable to operate at or below the e voltage. Above G O the storm loss becomes an important factor. Cal- culations should generally be made from formulae for each special case. To find the voltage at any altitude multiply the voltage found above by the 5 corresponding to the altitude, as given in Table LXXXII. 2 Kilovolts between lines corresponding to e at 25 deg. C. and 76 cm. ba- rometer. Conductors arranged in an equilateral triangle. CORONA CALCULATIONS FOR TRANSMISSION LINES 211 TABLE LXXXI. CORONA LIMIT OF VOLTAGE l Kilovolts between Line Three-phase Sea Level and 25 deg C WIRES Size B & S u Cir Mils Diameter, inches Spacing, feet 3 4 5 6 8 10 12 14 16 20 4 204 51 54 56 58 60 62 64 65 66 68 3 229 59 62 64 66 68 70 72 74 76 2 258 69 70 74 76 78 80 82 84 1 289 75 77 81 83 86 88 90 92 325 85 89 92 95 97 99 102 00 365 94 98 102 105 107 110 113 000 410 109 113 116 119 121 124 0000 460 120 125 128 131 134 138 To find the voltage at any altitude multiply the voltage found above by the 5 corresponding to the altitude, as given in Table LXXXII For single phase or two phase find the three-phase volts above and multi- ply by 1.16 TABLE LXXXII ALTITUDE CORRECTION FACTOR AT 25 deg. C. Altitude, feet 5 Altitude, feet 5 500 1,000 1 00 98 0.96 5,000 6,000 7,000 82 79 0.77 1,500 2,000 2,500 0.94 92 91 8,000 9,000 10,000 0.74 0.71 68 3,000 4,000 , 0.89 86 12,000 14,000 63 58 Corona is generally thought of as affecting only very high voltage transmission lines and of little other practical importance. It may, however, exist at almost any voltage, as it depends not only upon voltage but also upon the configuration of the electrode and the spacing. It will exist in cables, on insulators, coils, 1 Kilovolts between lines corresponding to e at 25 deg C. and 76 cm. ba- rometer. 212 DIELECTRIC PHENOMENA switches, etc.; in short wherever air is present, and where damage may be done by mechanical bombardment of small streamers, and by electrochemical action (ozone and nitrous oxide), unless means are taken to prevent it. In most cases its prevention is fairly simple. This is further treated in Chapter X. CHAPTER X PRACTICAL CONSIDERATION IN THE DESIGN OF APPARATUS WHERE SOLID, LIQUID AND GASEOUS INSULATIONS ENTER IN COMBINATION As important as the quality of the dielectric is the configuration of it and of the electrodes. It is also of importance in combining dielectrics of different permittivities to see that one does not weaken the other by causing unequal division of stress. It is possible to cause breakdown in apparatus by the addition of good insulation, dielectrically stronger than the original insulation. Case 1. Breakdown. Caused by the Addition of Stronger Insulation of Higher Permittivity. As an example take two Pxessboard FIG. 175. Causing break-down by the addition of insulation. parallel plates rounded at the edges and placed 2 cm. apart in air, as in Fig. 175 (a). (1) Apply 60 kv. (max.) between the plates. The gradient then is 60/2 = 30 kv./cm. max. (neglecting flux concentration at edges). As a gradient of 31 kv./cm. max. is required to rup- ture air there is no breakdown. u 213 214 DIELECTRIC PHENOMENA (2) Remove the voltage and insert between the plates a sheet of pressboard 0.2 cm. thick, as in Fig. 175(6). The constants of pressboard are k = 4 '.rupturing gradient = 175 kv./cm. max. / Z p = 0.2 cm. For air k = l^rupturing gradient = 31 kv./cm. Apply now the same voltage as before. The addition of the pressboard of higher permittivity has increased th * capacity of the combination and, therefore, the total flux and the flux density in the air. The gradient has also been increased. The combina- tion may be considered as two condensers in series. Where cj. = capacity of air condenser, 02 = capacity of press- board condenser; e\ = voltage across the air condenser, 62 = voltage across the pressboard condenser; the total flux is therefore, -y ei = y e% g zss g 2 ~f" 6l p _ _ _ i _ = KO 61 Mi + feA *A + Wi = 60 - 58.4 1.6 Then tfl - -^--^ . 32.5 br./oin. max. The air breaks down as gi is higher than the critical gradient, causing breakdown of air. As the broken down air is conducting, most of the applied voltage is placed on the pressboard. Thus, after the air ruptures, the gradient on the pressboard is: fiO g'z 7fo = 300 kv./cm. max. CONSIDERATION IN THE DESIGN OF APPARATUS 215 This is much greater than the rupturing gradient of pressboard and causes it to break down. Therefore, the 2.Ocm. space, which is safe with air alone, is broken down by the addition of stronger insulating material of higher permittivity. The stresses on this combination could have been calculated directly from (16a), Chapter II. Another and convenient way of looking at this is as follows: volts Flux - "flux resistance" or "elastance ?; S is termed the elastance and is the reciprocal of permittance. The reciprocal of the permittivity is termed the elastivity. For the given electrode arrangement, S is proportional to the elastivity and the length, as long as lines of force are practically straight lines. Let the relative elastivities be Air =1.0 Pressboard = 25 Let the absolute elastivity of the air be where a o a o a and 6 must be so chosen that the permittances between circles are equal. 228 DIELECTRIC PHENOMENA For any point p on the line A'lA'z (Fig. 1866), the potential to the neutral plane due to A' 2 is 26 Due to A'ij it is 4, . 2a t . 2(S' - 6) log6 ^ = 2^fc loge ~F FIG. 187 Graphical method of drawing lines of force between two cylinders. The total voltage from any point p to the neutral is 2(5' - 6) . 2b "" "" e np = t (. 2(5' - 6) . 2b\ - 2^5^ ^ lo S "" "" ^r -- g S 7 / It is desired to divide the field up into n equal voltages between the conductor surface and the neutral plane* The potential from the conductor to neutral is e n and is known Due to A' 2 : _zil i 2(r - ) ~ " CONSIDERATION IN THE DESIGN OF APPARATUS 229 Due to A' i : . log 2(5' - (r - )) - 8* - 8' - (r - z) 2-n-Kk ^ B r - z e n r-, Let ]8 be the fraction of the voltage e n it is desired to place be- tween the neutral plane and any point p on the surface under consideration, then (Fig. 1866) e np = e n & (Sf - 6) S' - (r - z) L{ loge r # In this problem I g 6 *: - L - 1 constant = F = anti-log _ . _ (anti-log ftF + 1) 6 is thus determined. If it is desired to find b for the first circle from the conductor ft = 0.9. l l "7.7 + 1 8.7 For the next circle j8 = 0.8 , 9.84 - ,, 62 = = L36 230 DIELECTRIC PHENOMENA Other values are found and tabulated in Table LXXXIII. a and R are thus found. The circles may now be drawn with radii fi, centers on A'lA'*, and intersecting A'iA'% b cm. from A\. TABLE LXXXIII. EQXJIPOTENTIAL SURFACES b a = S' - 6 B--AL a b a- 6 ab 1 b 900 8 90 1.00 8 00 8 00 0.9 b 1 1 HO 8 69 1 27 7 58 9 65 8 62 1 353 8 45 1.62 7 09 11 49 0.7 6 3 1 648 8 15 2 07 6 50 13 45 0.6 6 4 1 98 7 82 2 65 5 84 15 46 5 6 6 2 38 7 42 3 50 5 04 17 65 4 Z>6 2 81 7 09 4 65 4 28 19 90 0.3 & 7 3 29 6 51 6.65 3.22 21 40 2 6 8 3.80 6 00 10 35 2 20 22.80 0.1 6 9 4.34 5 46 21.15 1.12 23.67 610 4 90 4 90 00 00 24 00 F = 2.290 = constant z 0.1 S f = S - 2.3 = 9.8 The gradient at any point, and therefore the equigradient surfaces may be found as follows: The flux density at any point is D (Pages 21 and 23.) C n 6n = D = S'e n JL WE or for a given voltage, spacing and size of conductor, the term to the right is constant, and it follows: times a constant = J CONSIDERATION IN THE DESIGN OF APPARATUS 231 is the gradient at any point Xi cm. from A\ and #2 cm. from A' 2 . Putting x in terms of x% and the angle a between 2 and the line A'iA'%: cos =M FIG. 188. Method of plotting equigradient curves. TABLE LXXXIV. EQXTIGRADIBNT SURFACES a 30 60 90 120 150 180 g 21 4 #2 = 1 16 1 13 1 07 1.00 0.97 94 0.93 - 16 1 2 = 1.64 1 60 1 44 1.32 1 27 1.23 1.20 - 10.7 #2 * 2,91 2.85 2 25 2.00 1 85 1.75 1.74 g - 8.9 aj 2 = 4.90 3 40 2 71 2.37 2 19 2.06 2.02 g - 8.0 a? s = * J 4.0 3 08 2 59 2.38 2 26 2 20 * ,5.34 z a 4 94V-T 1 8 20 4 70 3,81 3.27 3.17 3 10 - 2.67 rc 2 i i 8 63 6.73 5 83 5.40 5 29 1 Such a gradient does not exist on this line and hence x% is imaginary. (See plot Fig, 8, page 15.) Gradient at Equidistant Points on the Conductor Surface Angle bet. horizontal A\A\ and Ime through point and conductor center 30 60 90 120 150 180 (7. ... .... 26 7 26 23.7 21 6 19 4 18 2 17.8 232 DIELECTRIC PHENOMENA (1) Find the maximum gradient at the conductor surface for 100 kv. between conductors. This may be found directly from equation (12a), pages 24 and 29, and is 26.7 kv./cm. (2) Find the gradient at six equidistant points on the con- ductor surface for 100 kv. between conductors. (See Table LXXXIV.) (3) Calculate the equigradient curves for gradients of 21.4, 16.1, 10.7, 8.9, 8.0, 5.34, and 2.67 kv. per centimeter at 100 kv. between conductors. This may be done from the above equation by putting g equal to the required gradient, and finding x% for given values of a. The results are tabulated in Table LXXXIV, and method of plotting is shown in Fig. 188. A complete plot of Case 9 is shown in Fig. 8, page 15. Note that in such a diagram, the permittance or elastance of each of the small cells bounded by sections of lines of force and equipo- tential surfaces is equal. Case 10. Dielectric Fields ia Three Dimensions. The field of a conductor arrangement which must be considered in three dimensions, as a rod and torus, rod through a plane, etc., is gen- erally represented on a plane figure in such a way that if the figure were revolved about its axis, the solid would be formed sur- rounded by its three-dimensional field. The small cells of the plane figure bounded by sections of lines of force and equipoten- tial surfaces would form cells in the solid of equal permittance. In the case of figures, as those for parallel wires, a wire in a cylinder, and parallel planes, it is possible to represent the field by considering only two dimensions. The height and thickness of the cells on the plane give constant permittance, or average , '." .- = constant. The third dimension is then the length thickness * ** of the wire and need not be considered in drawing these cells. In the case of the three-dimensional field, the cells on the plane must be of such a height and thickness that the solid cells have constant permittance, or where the cell is small hr , . -T- = constant. t This can readily be seen from Fig. 189. It is a general law that the cells must be so arranged that the stored energy may be a maximum or the permittance a maximum. In cases where the field need only be considered in two dimensions, it is thus possible, without great difficulty, to draw a field by a CONSIDERATION IN THE DESIGN OF APPARATUS 233 series of approximations in which the cells have a constant - or add up to maximum permittance. The lines of force must be normal to the electrodes and to the equipotential surfaces at the point of contact. This is also possible for a three-dimensional field, but extremely difficult because the cells must be drawn in such a way that the solid cells have constant permittance. The best way in which to determine a field that cannot be read- ' ily calculated is experimentally. If the electrodes are immersed in an electrolyte in a large tank made of insulating material, and a small current passed between them, equi- potential surfaces may be measured at equal voltage intervals on a plane through the axis of revolution by means of a galvanometer. 1 These surfaces correspond to the dielectric- equipotential surfaces. The lines of force may be drawn at right angles to these, so as to divide the field into solid cells of equal capacity (see above). It is difficult in practice to get results by this method when the problem includes several per- mittivities. Theoretically it would be possible to use a solid material to represent, for instance, the porcelain shell of an insulator, and the electrolyte to rep- resent the air. The resistivities of the two materials should then have the same ratio as the elastivities of porcelain and air. It is difficult to find a solid material with a resistivity in the order of that of an electrolyte. As a less exact experimental method, the lines of force may be obtained by mica filings and the problem then solved by approxi- mations. These methods may be developed into very useful ones for a study of flux control, etc. Case 11. Effect of Ground on the Permittance and Gradient for Parallel Wires. Such problems are* solved by taking the "images" symmetrically below the ground. 1 Fortesque has described this method. See A I.E.E , March, 1913. Much more exact results may be obtained than those shown in this paper. Bice, Solution of Electrostatic Problems, A.I.E.E., March, 1917. FIG. 189 Dielectric field three dimensions. 234 DIELECTRIC PHENOMENA Voltages between AB due A, B, Ai, BI are + C s= S' where the wires \ are far apart. / . . 2h =) log, The total voltage is e = B log>S2/i S (Bet. lines) log r a r a Where the wires are far apart the gradient is Q = 2h The problem for a number of wires may be solved in the same way. The fluxes from the different wires may then not be the same and the solution is more difficult as a number of simul- taneous equations must be writ- ten and solved. Case 12. Three-phase Di- electric Field with. Symmetrical ^ Groia and Unsymmetrical Spacings. The fluxes between conductors on a three-phase line vary sinu- soidally with the voltages. The instantaneous values of voltages may be added algebraically as FlG . ioo.-Effect of ground on ca- abov " , The &**> or pacity between parallel wires. mum values are found by geo- metrical addition. To illustrate: find the fluxes for three three-phase conductors in an equilateral triangle, and also for flat spacing. In order to greatly simplify the problem, the effects of ground or "images" will be neglected, and the conductors considered far apart. CONSIDERATION IN THE DESIGN OF APPARATUS 235 Then due to fluxes from A | B [ C , v u, 1 , f , AS , , . r 1 CB N ( fl ; ^AB ==: 0-7, g- C^A lOge + ^BlOge^T + ^C lOg 771") =6 Sin I E BC = ^ loge + ^& e sin (0 - 120) Only two of the three equations which may be written as above are independent, since the sum of the voltages must be zero. The other independent equation is (c) ^ A + *B + t A o Conductors Spaced in a Triangle o o (equilateral triangle). B C Substituting spacing S in (a) and (Z>) and solving for $ A , $ B , and \J/c ' (1.5 sin + 0.866 cos 0) Let 6(1.5 sin + 0.866 cos 6) ='e a (sin a) put = 90 and = and solve for e a and a . , A _ n , 1.16(irfcJC)e . , sin (0 - 150) = - '~7~~ sm ^ "~ ^ . .. OA . .j . ^ . sm (^ _ 30) = - v / sln (0_ _. _ = - ,- %- ^ c may be found in the same way, or for this particular case, A> $BJ & nc * to are ^qual by symmetry. For single phase: Therefore, when the wires are far apart, and with the same voltage 2 between lines, the three-phase stress is -/= times the single-phase stress. 236 DIELECTRIC PHENOMENA Flat Spacing A B C Putting >S ; S, and 2>S in a and b and o o o solving as before, 2irkKe _ ^ B = __ -- --- sm y _ 150) \/3 log, - -0.58 log 2 . , gm (0 _ V3 log, ^-0.4 The flux, and therefore the stress, when the wires are far apart, Sf is greatest on the middle wire. For - = 500 it is 4 per cent. greater than on the wires with the same S and triangular spacing as above. ^, and \l/ c are 6 per cent, lower than for the triangular spacing. The gradients vary in the same way. Corona, therefore, starts on the center wire at a 4 per cent. lower voltage, and on the outer wires at a 6 per cent, higher volt- age than for triangular -sjjacings. Case 13. Occluded Air in Insulation. It is interesting to estimate the effect of occluded air in solid insulation. Assume that in the process of manufacture air bubbles have formed in a sheet of rubber insulation. The sheet is 1 cm. thick. The " bub- bles" are thin compared to the rubber, and long in the direction of the length of the sheet. It is estimated that the largest ones are 0.01 cm. thick, and 0.1 cm. long and wide. The electrodes which the rubber insulates may be assumed as being practically parallel planes. The working voltage is 40 kv., or the stress is 40 kv./cm. effective in the rubber. As the air bubbles are not thick enough to greatly disturb the field, the same flux passes through the air as through the rubber. The permittivity of the rubber is 3, The stress on the air is, therefore, 3 X 40 = 120 kv./cm. effective. Air breaks down at 21.2 kv./cm. effective at atmospheric pres- sure. It seems probable that these bubbles will break down, even after allowance is made for the extra strength of thin films, and a possible pressure higher than atmospheric. See pages 61, 196 and appendix. It is probable thafc the golid insulation would soon break down on account of heat and chemical action. Case 14. General. (a) Estimate the visual corona voltage when wires are wet. Compare with the visual corona voltage when wires are dry. CONSIDERATION IN THE DESIGN OF APPARATUS 237 Calculate g v from the formula on page 67, Chapter III. Insert the value in formula (20). Maximum e v to neutral is thus found. If the voltage used is a sine wave, reduce to effective kv. by dividing by \/2- For a three-phase line the voltage between wires may be found by multiplying by V3; for a single-phase line, by multiplying by 2. Compare with dry visual critical voltage calculated from equation (20); page 43. (6) At what voltage will the above wires spark over wet and dry single phase; three phase? Estimate dry spark-over voltage from equation given on page 83, Chapter IV. Estimate wet arc-over voltage by assuming needle gap spark-over. (c) Calculate the dry arc-over curve for a 10-cm. sphere (grounded) at d = 0.90, and spacings from 1.5 to 10 cm. Use equation (136), Chapter IV. Estimate a wet spark-over curve as outlined for spheres on page 105, Chapter IV, (d) What is the voltage required to puncture 0.5 cm. of paper insulation when the time of application is limited to 1/100 second? In 100 seconds? Use equation on page 179, Chapter VII, of the form e& = g s X thickness. (e) Estimate the loss per cubic centimeter at 1000 cycles in a piece of varnished cambric, at 5.0 kv./mm., 25 deg. C. Use equation page 185, Chapter VII. (/) What is the breakdown gradient of a piece of porcelain 2 cm. thick? where t = thickness in mm. g = gradient in kv./mm. (eff.) (See Chapter VII, page 174.) DATA APPENDIX 1. MEASURED CORONA LOSS Indoor Line 60-cycle The current and watts given are measured values due to corona, divided by the total conductor length in kilometers. Corrections have been made for transformer and leads. The voltage is given to neutral. As these measurements were made on a single-phase line, the voltages between wires were twice the value given. To obtain kva. per km. of conductor multiply amps, per km. by volts between lines. CORONA Loss INDOOR LINE 60-CYCLE Test 10B Test 11J5 Eff kv. to neutral, e n Amp. per km Loss kw /km , # Eff kv to neutral, e n Amp, per km Loss kw /km , p 10 52 12 52 14 80 17 10 07 51 1 40 3.20 13.7 16 7 18 1 19 9 070 33 92 1 11 1 64 18.20 19 60 22 30 24 90 225 310 4,02 6 83 9.44 15.03 24 7 29 3 33 2 36 3 0,100 150 0.189 223 3.95 6 90 10 40 14 20 27.20 29 70 28 00 25 90 395 404 0.342 20 63 22 40 16 80 39 7 44 47.3 50 2 0.268 325 0.380 18.75 26 73 34 20 23.60 20 80 18.40 0,263 11 80 7 16 4.14 45 2 41 5 37.4 350 293 0.238 29.20 22.20 15.69 16 10 1 98 31.0 0.163 8 08 27 22 3 0.128 082 5 29 2 53 Spacing, 15 25 cm. Kadius, 032 cm Total? cond. length, 0,0838 km. d 1.02, Spacing, 30.5 cm. Kadius, 0.032 cm. Total cond. length, 0.0838 km. 5 1.02. 238 DATA APPENDIX 239 Test 1W Test 15B Eflf. kv to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 19 5 0.051 96 17 3 __ r - 35*" 24.3 071 1 78 23 7 059 1 17 29.6 099 3.23 ^MrVT^ 078 2 34 34 133 "4 9>5~~- 36 1 109 3 92 38 146 6 49 42 2 5 76 43.0 9,13 49 8 166 9 26 46 7 0.196 12 51 56 7 200 13 21 52.4 224 16.35 62 5 223 16 70 57.5 21 00 66.5 246 20 00 62.5 285 26 25 71 4 .... 24 35 68.3 327 34 40 78 6 310 30 95 73.1 359 40 60 84.4 0.322 37 20 79.1 0.385 50 50 89 4 345 41 90 84.0 59 50 95 4 50 50 90.0 0.430 72.00 99 3 395 58 60 93.6, 460 83 10 91.0 0.369 45 60 102.0 510 93.40 81 6 0.310 34.10 67.9 21 55 52 1 0.177 10 46 39.1 126 4.44 27.0 068 1.74 Spacing, 61 cm. Eadius, 0.032 cm. Total cond. length, 0.0838 km 5 - 1.03. Spacing, 91,5 cm. Radius, 0.032 cm Total cond. length, 0,0838 km. 5 - 1.012. 240 DIELECTRIC PHENOMENA Test 20B Test 21B Eff kv to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 17 8 21 19 8 81 24 6 1 29 24 5 1 15 30 1 2 17 27 2 2 02 36.2 " 110 3.71 30 7 2 19 42 128 5 16 34 8 3 42 47 159 6 94 39 8 129 3 86 53 2 190 9 80 44 8 156 5 04 62 233 14 60 50 4 0.177 6 47 67 6 258 19 23 55 1 212 8 45 73 4 273 21.12 60 6 0.234 10 80 78 1 26 70 64 6 0.246 12 40 85 2 346 33 10 70 0.266 15-. 10 93 2 0.385 42 70 77.9 310 19.30 100 2 51 70 87.6 26 60 87 0.350 35 60 94.3 32 60 76.1 0.298 25.00 101.5 41 00 65.2 250 15.95 49 4 178 7 44 40,1 0.114 4 55 Spacing, 122 cm. Radius, 0.032 cm. Total cond. length, 0.0421 km. 6 - 1.018. Spacing, 183 cm. Radius, 0.032 cm, Total cond. length, 0.0342 km. d 1.012. DATA APPENDIX 241 Test 22B Test 24B Eff kv to neutral, e n Amp per km Loss kw /km. , p Eff kv to neutral, en Amp per km Loss kw /km , p 20 7 72 20 1 24 24 5 1 01 25 3 98 27 2 1 21 32 1 84 30 9 1 98 36 103 3 18' 34 6 100 2 34 41 120 4 52 40 1 121 3 57 45 7 138 6 11 45 2 149 4 53 50 3 8 30 50 3 171 5 71 57 185 11 57 55 1 7 43 62 2 210 15 10 60 2 215 9 13 67.3 240 19 15 64 6 230 11 05 72.4 266 23 20 69 5 11 99 77 5 290 27.50 78 5 16 37 82 3 32 10 87 5 345 23 00 87 8 37 90 94 2 380 26 00 92 5 43 80 103 2 417 34 50 97 3 50 80 100.5 55 60 79.0 28 70 65.0 17 10 52 7 9 90 Spacing, 274.5 cm. Radius, 0.032 cm. Total cond. length, 0.0342 km. 5 1,012. Spacing, 91.5 cm. Radius, 0.057 cm. Total cond. length, 0.0818 km. 5 = 1.0009. 242 DIELECTRIC PHENOMENA Test 2GB Test 28B Eff kv to neutral, em Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 1 20 37 10 6 23 2 053 98 14 2 29 2 24 16 1 0.18 32 8 3 36 18.4 43 37 1 124 5.14 20 2 0.98 41 1 141 6 60 22 2 061 1 34 46 7 173 9 90 24 069 1 83 51.3 202 12 32 25 072 2 20 57 1 232 18.30 27 0.087 2 93 61.1 262 22 30 30 2 120 5.00 66 2 290 28.40 34 0.157 7.88 72.0 332 36 60 36.7 178 10.30 75.7 334 40 80 36 7 0.181 10 10 80.7 ... .... 50 50 40 7 212 14 80 85.0 413 56.50 44,5 265 , 20.30 88.7 0.431 64 00 47 1 0,298 24 80 91 0.464 71.40 51 7 369 35 20 96 5 0.515 83.40 49 6 0.342 30.80 101 562 104.00 43 0.251 18.20 82.8 Q.396 54,50 74 7 333 39 00 69 7 33.00 60 255 22.70 Spacing, 61 cm, Radius, 057 cm. Total cond, length, 0.08186 km. S 1,002. Spacing, 30.5 cm. Radius, 0.057 cm. Total cond. length, 0.0818 km. B 0,993. DATA APPENDIX 243 Test SOB Test 32B Eff kv to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 21 7 18 22 5 21 25 6 92 27 2 049 31 31 5 2 45 32 5 062 1.41 36 2 4 30 37 2 086 2 70 40 5 138 5 80 41.1 100 3.68 45 7 156 8 60 45 6 123 5.03 49 7 180 11 70 50 3 146 7.35 54 2 204 15 30 55.0 0.178 10 18 59 5 238 19 50 60 194 13 50 64 0.269 24 60 65 7 222 17 40 68 2 290 29 70 72 257 23 20 73 322 36 30 77 2 278 27 60 78.5 352 45 20 82 5 0.298 31 40 83.5 384 54 00 89 2 40 00 88 2 0.441 63 00 92 2 44.00 95 486 76 00 85 2 35.80 96.5 500 81 20 70.0 20.80 100 530 92 00 61.7 14.32 103 600 114 30 90.2 0.459 60.20 , 79.5 356 45 30 75.2 0.319 38 60 65.5 26.20 51.7 13 40 t Spacing, 61 cm. Radius, 0.071 cm. Total cond, length, 0.0815 km. 5 - 0.98. Spacing, 91.5 cm. Radius, 0.914* cm. Total cond. length, 0.0815 km. 8 1.002. 244 DIELECTRIC PHENOMENA Test 33.B Teat 41J3 Eff. kv. to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 24 7 31 28 3 29 8 1 53 35 5 071 2 72 32 6 * 2 45 41 0.108 4 90 35 6 3 50 48 6 184 10 40 39 3 4.96 53 7 208 13 25 43 7 6 37 59 0.234 17 50 47 5 9 57 63 8 0.265 23 40 51 5 12.9 69 4 0.306 30 02 56 3 15 5 73 6 0.353 35 70 60 2 20 8 71 9 325 34 10 65 5 34 8 60.1 244 19 85 67 29 6 54 2 210 13.65 54.4 15 3 59.9 250 19 35 57 224 16.30 47 161 8 87 Spacing, 61cm. Radius, 0,0914cm Total cond. length, 0.0815 kin. d = 1.006. Spacing, 61 cm. Radius, 0.105 cm. Total cond. length, 0423 km. 5 * 1.001. DATA APPENDIX 245 Test 455 Test 47B Eff kv to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 22 3 06 45 080 37 25 8 12 50 100 74 29 7 34 54 5 104 1 90 35 7 1 41 60 5 5 76 39 5 2 70 65 7 152 9 13 44 2 4 78 70 5 0,174 12 60 50 2 8 10 75 5 205 16 30 54 10 70 79 230 18 75 59 5 14 70 87 26 80 64 5 19 50 91 7 31 40 69 24 80 96 5 38 20 74 30 10 93 5 321 34 10 79 7 37 20 90 29 80 82 7 43 40 82 21 70 88 7 56 20 75 8 16 20 98 59 00 58 4 22 99 7 80 50 42 6 49 103 84 50 40 24 86.7 52 20 75 5 32 70 Spacing, 61 cm. Radius, 0.164 cm. Total cond. length, 0.0185 km. 6 = 0.996. Spacing, 91 5 cm. Radius, 0.256 cm. Total cond. length, 0.0815 km. 5 = 0.996. 246 DIELECTRIC PHENOMENA Test 4&B Test 495 Eff. kv. to neutral, e n Amp per km Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 44.1 61 40 5 1 16 47.2 1.11 44 5 3 -13 51.7 < 3 87 43 2 27 54.5 5.90 46 8 5 70 60.8 10 60 50 6 12 30 67 2 17 15 55 6 19.25 71.5 20 70 58 8 75 5 26.70 53 8 16.05 81.7 33 30 49.6 9.70 76 6 27 10 45,7 5 27 78.5 29 40 43 2 2 82 74.0 23 90 39.3 1.23 69.5 18 30 68 16.55 58 2 8 10 52.7 4 10 Spacing, 61 cm. Radius, 0.256 cm. Total cond. length, 0.0815 km. 5 - 1.00. Spacing, 30.5cm. Radius, 0.256 cm. Total cond. length, 0.0815 km. 5 - 0,996. DATA APPENDIX 247 Test 5 IB Test 54# Eflf kv to neutral, e n Amp per km. Loss kw /km , p Eff kv to neutral, e n Amp per km Loss kw /km , p 62 5 68 72 159 190 220 9 15 14 55 20 10 25.5 31.8 37.7 051 0.06 78 261 28 45 42.7 0.30 87 3 318 40 20 47.1 0.30 91 5 49 70 57.0 49 82 72.8 34 60 22 10 63 2 69 7 1 03 1.81 56 61.5 5 65 10 20 76 5 78 7 152 164 5.08 6 48 67 2 70.2 15 75 19 30 84.5 89 3 0.184 210 12 22 17 20 95 99 1 102 2 238 263 23.90 28 40 31 90 97 2 92 87.0 76 7 82.0 72 1 26 00 20 90 16 50 5 82 9.10 2 67 Spacing, 61 cm. Spacing, 91.5cm, Radius, 0.333 cm. Radius, 0.464 cm. Total cond. length, 0.0817 km. Total cond. length, 0.0825 km. S ** 0.999. S 0.982. All of the above tests were taken at a temperature of about 25 deg, C. MEASURED CORONA LOSS Outdoor Line 60 cycle Columns 1, 2, and 3 are actual measured values and include transformer and lead losses. Column 4, the actual corona loss, for the length of line used in the test is obtained from Column 3 by subtracting transformer and lead losses. These tests were made on comparatively long single-phase lines out of doors, and the conductor surfaces, etc., were not in as good condition as in the case of the indoor line. Transformer losses 248' DIELECTRIC PHENOMENA for several temperatures are given. The voltage values are ef- fective between lines. Test No 146, Line A 1 Test No 18, Line A Kv bet lines Amp Kw Kw line loss, p Kv bet lines Amp Kw Kw line loss, p 63 5 056 07 01 80 040 12 0,01 80 5 077 12 02 90 100 ,0 16 02 90 1 092 15 02 101 1 107 20 04 107.5 113 30 12 112 113 25 05 115 2 121 35 14 121 6 123 30 06 126 2 135 63 37 129 5 131 35 07 134 2 146 85 55 140 146 49 16 142 5 154 1 29 95 150 160 76 0.38 150 164 1 95 1.45 160 172 1 60 1 17 158 173 2 69 2 25 152 162 90 51 166 1 185 4 00 3 48 164 2 174 2 00 1 55 165.0 1.83 3 51 3 02 172 187 3 40 2.90 173 7 196 5 00 4 45 183 2 205 5 60 5 02 163.4 184 2.70 2.23 188 2 210 6 92 6.30 170 4 193 4,20 3 67 196 4 0.223 9 02 8.42 181.0 198 6 06 5 42 202.2 237 11 06 10 36 203 0,251 12.84 12,04 206 242 12 90 12 09 199 2 243 11 50 10 73 187.2 211 6.95 6 34 193 4 227 9 10 8.49 196 4 225 9,60 8.90 176.4 197 4 74 4.17 Total conductor length, 109,500cm. 165 6 184 2 70 2,21 Spacing, 310 cm. 162 8 180 2 38 1 81 No. 3/0 7-strand hard-drawn copper- 154 4 169 1.28 0.85 weathered cable, diam. 1.18 cm. 166.0 0.176 2 94 2 45 Temperature, wet, 16 deg. C. dry ; 18.5. 184 4 198 6.49 5 87 Barometer, 75 5 cm. 172.0 193 3 85 3 31 Bright sun, wind. 160 177 2.03 1.57 Test No. 146, Lino A 146 2 162 0.80 42 Total conductor length, 109,500 cm. Spacing, 310 cm. 138.0 0.150 52 0.19 No. 3/0 7-strand cable, dia. 1,18 cm. 127.6 0.137 0.40 12 Temperature, wet, 24 deg, C. 122.5 129 0,33 08 dry, 30 deg. C. 111.2 117 25 04 Barometer, 75.7 cm. 101 0.105 20 0.03 Hazy. curve was taken after the line had been standing idle over a month in the summer The "going; up" points show an excess loss due to dust and dirt on the conductor. This disappears at high voltage and does not show in the "coming down" readings. DATA APPENDIX 249 Test No 102 Kv bet lines Amp Kw. Kw line loss, p 201 232 6 05 6 65 211 277 9 10 8 63 189 210 3 54 3 19 181 8 200 2 36 2 04 170 8 189 1 10 80 160 176 60 36 149 162 0.36 16 201 231 6 15 5 75 149 162 39 19 140 5 0.150 29 12 135 5 145 25 10 124 5 0.131 20 08 113 5 0.118 16 08 102.3 103 13 07 Total conductor length, 109,500 cm. Spacing, 310 cm. No. 3/0 7-strand H D copper- weathered cable, diam 1.18 cm. Temperature, wet, 1 dry, 1 Barometer, 7.47 cm. Cloudy. 250 DIELECTRIC PHENOMENA Test No 84, Line A Test No 105, Line A Kv bet lines . _- Kw line Amp. Kw , F loss, p Kv bet. lines Amp Kw Kw line loss, p 120 138 24 15 79 8 0.080 03 01 129 150 30 19 90 7 093 04 01 160.0 0.175 0.78 61 101 5 106 06 02 181 202 3 65 3 40 109.5 0.114 08 0.03 189.0 212 4 65 4 36 120.5 0.127 10 0.04 203,0 0.237 7 84 7 48 130 139 14 06 213 252 11 20 10 78 141 5 154 19 09 205 0239 870 8.18 147.0 0,165 0.21 08 153 6 0.168 0.25 12 Total conductor length, 108,500cm. 159.0 0.178 0.30 0.16 Spacing, 310 cm. 169 8 199 51 35 No. 3/0 7-strand cable (H, D. copper- 174 190 0.70 53 weathered), 1.18 cm. Temperature, wet, 1 deg C. 181 198 1.20 1.02 dry, 3 deg, C. 186 2 0.204 1.74 1.55 Barometer, 75.2 cm. 192,6 0,212 2.70 2,49 Cloudy. 200 6 221 4.00 3,77 208 6 0.237 5 60- 5.34 216.0 0.247 7.40 7.13 221 259 9.00 8,70 227,0 0.271 11.00 10 66 234 288 13.60 13 25 189.0 0.210 2.30 2 10 195.0 217 3,10 2.88 203.8 0.229 4.96 4.72 212.0 0,242 6,70 6.44 219.0 0.257 8.60 8,31 Total conductor length, 109,500 cm. Spacing, 310 cm. No. 3/0 7-strand H. D. copper- weathered cable, diam. 1.18 cm. Temperature, wet, 13 deg. C, dry, 13 deg, C. Barometer, 76.2 cm. Bright sun, no wind, snow on ground. DATA APPENDIX 251 Test No 100, Line B Test No 73, Line B Kv bet lanes Amp Kw Kw Ime loss, p Kv bet lines Amp Kw Kw line loss, p 67 02 02 43 016 77 025 03 02 60 022 88 '0 028 05 02 69 7 026 08 0.06 98 9 0.035 07 03 80 6 0.030 10 0.07 109 5 040 12 07 90 5 034 15 11 119 5 043 22 14 101.5 038 30 26 128 050 42 32 91 034 09 0.05 137.0 0.054 90 78 90 5 034 10 0.06 144 060 1 94 1.80 70,3 0.026 06 0.04 161 2 078 4 50 4.31 101 6 0.038 0.17 0.12 153 070 3 04 2 88 101 6 038 17 0.12 173.8 0.090 6 60 6 47 109 5 0.041 40 0.36 185.0 0.103 8 72 8 36 105 5 040 14 0.09 200 0,106 11.90 11 59 115 040 0.14 0.09 185.0 103 8.76 8 50 115 0425 88 0.82 159.0 078 4.10 3.92 121.5 0.048 0.16 0.09 139 058 1 22 1 10 126 5 0.053 2 00 1 93 161.2 0.080 4.70 4.51 130 5 055 2 48 2 40 211.8 0.135 14.80 14.46 140.5 064 3 70 3 61 144.5 0.073 4.26 4.16 Total conductor length, 29,050 cm. 70 5 03 0.00 Spacing, 91,4 cm. 91 5 030 06 0.02 0.375- in. galv, steel cable, diain. 106 0.038 0.18 0.13 0.953 cm. 150.0 0.078 4 80 4 69 Temperature wet, 1 deg. C. dry, 1 deg, C. 156.4 083 5 80 5 68 Barometer, 74.7 cm, 161 0.089 6.72 6.67 Cloudy. 166.0 0.093 7.50 7 36 Total conductor length, 29,050 cm. Spacing, 91.4 cm. 0.23-in. galv, steel cable, diam. 0.585 cm. Temperature wet, 1 deg. C. dry, 3 deg. C. Barometer, 75.2 cm. Cloudy. 252 DIELECTRIC PHENOMENA Test No 79, Line B Test No 80, Line B Kv bet lines Amp Kw Kw line loss, p Kv bet lines Amp Kw Kw. line loss, p 213 105 8 64 8 38 81 029 0.07 0.04 205 010 7 68 7 40 91 032 0.09 05 202 0.094 7.40 7 13 100 5 035 12 07 186.0 088 6 00 5 80 110 5 0.038 16 11 181 081 5 00 4 80 120 5 041 40 34 168 4 072 3 96 3 81 130 5 048 1 30 1 22 159 6 063 3 00 2 88 139 5 055 2 25 2 17 150 058 2 24 2.13 153 067 3 20 3 09 138 048 1 14 1.06 160 0.075 4 40 4.28 120 043 20 14 172 084 5 70 5.54 120 26 20 181 094 7 00 6 82 110 071 19 14 192 0.103 8 50 8.28 99 068 0.13 09 199 109 9 40 9 15 213 124 11 70 11 38 Total conductor length, 29,050 cm. Spacing, 244 cm Total conductor length, 29,050 cm. P 23-m. galv. steel cable, diam. 0.585 cm Spacing, 152 cm. 23-m. galv. steel cable, diam. Temperature, wet, 1 deg. C. 0.585 cm. dry, 3 deg. C. Temperature, wet, 1 deg, C. Barometer, 72 5 cm. dry, 3 deg. C. Cloudy. Barometer, 72.5 cm. Cloudy. DATA APPENDIX 253 CORONA Loss OUTDOOR LINE GO-CYCLE Test No 125, Line B Test No 126, Line B Kv bet lines Amp Kw Kw line loss, p Kv bet lines - Amp Kw. Kw line loss, p 80 025 06 05 100 031 12 09 88 031 13 11 110 037 22 17 101 037 32 29 119 041 44 36 110 041 74 68 131 0.050 1 36 1 22 120 050 1 67 1 59 142 056 2 38 2 16 128 056 2 56 2 44 151 065 3 23 2 92 140 067 4 00 3 80 160 074 4 20 3 78 150 08 5 42 5 12 171 082 5 45 4 93 159 6 09 6,86 6 46 181 09 6 56 5 89 168 4 101 8 30 7 80 194 102 8 20 7 34 181 112 10 36 9 68 202 111 9 26 8 30 190 122 12 24 11 44 212 117 10 84 9.74 201.0 134 14 68 13 61 222 128 12 44 11 18 213 148 17 28 16 14 231 135 13 80 12 38 206 144 15 76 14 72 225 129 12 88 11 58 196 6 0.128 13 60 12 70 217 0,124 11 64 10 45 186 2 0.117 11 44 10 69 205 112 9 70 8 70 175 103 9 20 8 59 196 6 104 8 56 7 68 165,6 * 096 7 76 7 27 186 6 096 7 32 6 56 153,4 083 5 92 5 57 176 086 6 12 5 51 143 074 4 56 4.33 165 0.078 4 96 4 49 134 064 3 34 3 18 156 4 069 3,96 3.59 123,0 0.053 2 00 1.90 142 4 056 2 46 2 24 114 0,044 1.00 94 134 051 1 60 1 45 104 0.038 38 34 125 044 82 71 Total conductor length, 29,050 cm. Total conductor length, 29,050 cm. Spacing, 91.4cm. Spacing, 183 cm. No. 4 H D. copper wire, diam. 0.518 No. 4 H. D. copper wire, diam. cm 0.518 cm. Temperature, wet, 5 deg. C. Temperature, wet, 5.0 deg. C. dry, 4.6 deg. C, dry, 4.5 deg. C. Barometer, 75.9 cm. Barometer, 75.9 cm. Cloudy, slight breeze. Cloudy, slight breeze. 254 DIELECTRIC PHENOMENA Test No 137, Line B Test No 138, Line B Kv. bet. lines Amp Kw Kw. line loss, p Kv bet. lines Amp. Kw. Kw line loss, p 80.0 05 02 79 2 06 03 90.5 025 11 06 91 2 025 12 07 100.5 029 35 0.26 99 9 0.027 26 0.18 110 7 0.037 95 78 111 4 036 08 65 121.0 0.044 1.42 1 19 120 8 039 1 22 1 06 131 051 2.11 1 76 121 5 049 1 90 1 59 141 5 056 2.70 2.26 141 055 2 3.0 2 20 150.8 0.064 3 24 2.72 149 0.059 2.80 2.34 161 072 4 05 3.40 161.0 066 3.40 2,85 172 078 4.80 4 05 171 4 074 4 20 3.53 183 084 5 60 4 73 181 4 079 4 80 4.05 196 093 6.60 5.59 192 085 5.60 4.73 205.0 0.102 7.60 6 44 202.2 0.092 6 56 5.67 202 0.098 7 30 6 19 214 4 0.11 7.50 6 35 186 0.087 6.00 5 08 197.0 0.089 6.10 5 15 165 0.075 4 30 3.63 174 0.076 4.40 3 71 145 0.061 2.86 2.40 153 2 063 3.00 2.51 124 0.047 1.75 1.46 134.4 0.051 2.00 1.67 103.0 032 60 0.47 Total conductor length, 29,050 cm. Spacing, 488 cm. No. 8 new H. D. copper wire, diam. 0.328 cm. Total conductor length, 29,050 cm. Spacing, 366 cm. No. 8 new H. D. copper wire, diam. 0.328 cm. Temperature, wet, 1.5 deg. C. dry, 1.5 deg. C. Temperature, wet, 1.5 deg. C. dry, + 1.5 deg. C. Barometer, 75.5 cm. Barometer, 76.6 cm. Bright sun, slight breeze. Bright sun, slight breeze. DATA APPENDIX 255 Test No 92, Line B Test No 95, Line B Kv bet lines Amp Kw Kw line loss, p Kv bet lines Amp Kv/. Kw line loss, p 27,5 008 222 115 8 80 7 00 34 5 009 199 8 104 6 80 5 38 39 5 Oil 181.0 089 5 36 4 24 44 5 013 02 01 158 076 3 80 2 98 51.0 015 05 04 140,0 064 2 84 2 24 56 5 017 0.10 09 120 053 1 92 1 44 61 5 019 0.22 20 102 . 1 21 96 66 5 023 37 31 91 5 034 93 75 71.0 0.024 49 40 79 5 028 63 51 76 028 0,60 49 68.7 021 63 52 83 032 0.81 66 60 017 18 16 90.5 101 110 5 120 5 131 5 144 5 158 170 0.037 041 050 055 060 0,068 081 0,086 1 07 1 43 1 80 2.30 2 80 3 50 4 40 5 30 88 1,17 1 46 1 88 2.28 2 84 3 57 4 33 50 014 Total conductor length, 29,050 cm. Spacing, 550 cm 0.066 m. galv, steel wire, diam. 168 cm. Temperature, wet, 1,0 deg. C. dry, aO deg. C. Barometer, 75.0 cm. Cloudy, no wind. 181,0 094 6.18 5,15 190 0,099 6.70 5,43 204,0 0.110 8,00 6 50 215,0 117 9.00 7 30 222 123 9 64 7,84 Total conductor length, 29,050 cm. Spacing, 410cm. 0.066-in. galv. steel wire, diam. 168 cm. Temperature, wet, 5 deg, C, dry, 2.0 deg, C. Barometer, 75.0 Cloudy, no wind. 256 DIELECTRIC PHENOMENA TRANSFOEMBR Loss Kv Amperes Kw. Kv. Amperes Kw. 101 5 0.008 71 5 0.005 0.02 131.5 0.010 15 82 0.006 0.03 147.3 0.011 25 97 0.007 0.05 112 0.008 0.06 163.8 0.013 0.42 132 8 009 09 181 5 0.014 54 201 8 0.016 69 149.0 0.010 0.12 178 4 0.013 18 30-C 201 0.014 22 223.0 0.016 30 3C. 2. IXC. TESTS (Tests from Peek, A.I.E.B., June, 1916, unless otherwise noted) Spark-over and Corona in Air Sphere Gaps. The d.c. voltage required to spark-over a given spacing is the same as the maximum a.c. TABLE 1. A.c AND D c. SPARX-OVEB VOLTAGES OP 2/0 NEEDLES IN AIR Spacing, cm Kilovolts 00 cycle ("max ) Kilovolts dc. 5 1 51.0 52.0 7 6 62,5 63 10 2 76 5 73 5 12.7 88.3 82 5 15.3 , 98.3 90 5 5 = 0.98 Hum. 34 per cent. TABLE II. D.c. AND A.c. VISUAL CORONA AND SPARK-OVER VOLTAGES (Concentric Cylinders Normal Air Density 6= R f Corona Spark-over radius outer oyhnder, wire radma, cm. JR/r 60 cycle alc. JCV DC. + D.c. A.c. Qvm&x D.c. {J 00 cy kv D.c. 4- D.o. cm. (max.) kv. kv. kv./cm kv /cm. max kv kv. 3 81 0038 1000 4.9 6.4 0.4 186.0 244.0 Vibrates be- 3 81 0129 295 8 4 8 4 8.3 113.0 113.0 70.0 foro sparkover 3 81 0.0573 66 5 17.2 17 2 17 2 71 5 71 5 40 52 8 61 81 130 29 3 25.2 25.2 25 2 56 9 56 9 25 5 48.8 54 5 n 239 16.0 33.5 33 8 33.8 51.0 51.3 33 9 47.5 52.8 X 0,035 6.0 48.9 49.0 49.0 42 9 43.0 48.1 49.5 53.2 1 110 3 4 54.7 54.8 54.8 40.5 40.6 54.5 54.5 55.5 DATA APPENDIX 257 TABLE 111. D.c. AND A c. VISUAL CORONA VOLTAGES (Concentric Cylinders at Various Air Densities) R Ac radius outer r radius R/r 5 calc 60 cy DC. + DC Ac. calc. D.c. ffv D c. g v cylinder cm wire cm kv. (max ) kv. kv. gv (max ) H- kv./cm. kv /cm. 2 90 239 12.1 1 00 30 30.0 30.0 50.5 50.5 50 5 2 90 239 12 915 28 27.8 27 8 47 46.8 46 8 2 90 239 12 S57 26 3 20 2 44 2 44 2 90 . 239 12 824 25 7 25.5 43 3 42.9 2 90 239 12 797 25 1 25 1 42 2 42.2 2 90 239 12 720 23 1 23.1 .... 38 8 38.8 2 90 239 12 1 680 22 1 22 1 37 1 37.1 2 90 0.239 12 1 0.550 19 1 19 2 19 3 32 1 32.2 32 4 2 90 0.239 12 1 435 15 7 15 7 16 26 4 26 4 26 9 2 90 239 12 1 357 13 5 13 5 22 7 22 7 2 90 0.239 12 1 260 10.7 10 9 11 6 18 18.4 19 5 2 90 0.239 12 1 082 4 8 4 4 4 6 8 07 7 4 7 75 TABLE IV. COMPARISON OF RESULTS* Critical Surface Intensity* Kilovolts per Centimeter Alternating current Continuous current Diam. wire, White- head Peek White- head & White- head & Brown Farwell White- head & Brown Farwell em Brown H- - 074 81.2 80 7 80.3 76.0 75 7 80.8 76.9 090 76 6 76 76 71.9 71.6 76.1 72.0 107 72 9 72.3 72 5 68 9 68.3 72.4 69.8 0.125 69 9 69 2 69.6 66 2 65.5 69.3 67.2 0.166 64 8 64 1 64.8 61 9 61.1 64.2 62.9 231 59.9 59.1 60.1 57 6 56.6 59 1 58.7 l Whitehead, A.I E.E , Feb., 1917. See also Whitehead, A.I.E B., June, 1920. TABLE V. STJBFACE SPAKK-OVBR OF SUSPENSION INSULATOKS D c kv Insulator 60 cycle number kv (max ) cap H- cap 1 116 117 5 127.5 2 99,0 99.0 106 3 126.0 132 139.0 4 111 5 128 135 5 119 128 135 258 DIELECTRIC PHENOMENA D.c. Spark-over in Oil TABLE VI. D.c. AND A c. SPARK-OVER TESTS ON 2/0 NEEDLES IN No. 8 TRANSIL OIL AT 25 DEG. C. Needle gap, cm. 60 cycle kv. (max ) DC kv. (max ) 317 21 2 21 7 635 34 7 33 5 1 27 50 5 50 2 1 91 65 66 2 54 86 5 82 5 D.c. Strength, of Solid Insulation TABLE VII. VARIATION OF 60 CYCLE PUNCTURE VOLTAGE WITH TIME OF APPLICATION ON VARNISHED CAMBRIC Tests Between 2.5-in. Plates, IJ^-in, Radius Edge, in No. 6 Transil Oil Temperature, deg C. Sheets Thickness, mm kv (max ) Time, sec. 25 1 30 24.8 2.3 (12 mils) 21.3 12 19 5 17 3 17 7 41 5 15.9 198 14.2 900.0 100 1 30 14.5 2.0 13.2 7.0 12 6 11.0 12.0 25.0 10 8 620.0 9.9 1400.0 25 2 0.60 29.8 213.0 26.7 700.0 25.6 1418.0 25 3 0.90 53.0 8.0 45*2 51 5 42.5 80.0 41.7 138 38.9 370.0 37.1 905.0 25 4 1.20 69.3 4.0 65.0 13.0 64.3 15.0 55.8 39.0 53 80.0 50,8 155 47.3 580. o; DATA APPENDIX 259 TABLE VIII. VARIATION OF D.c. PUNCTURE VOLTAGE WITH TIME OF APPLICATION ON VARNISHED CAMBRIC Tests Between 2.5-in. Plates, 1%-in. Radius Edge, in No. 6 Transil Oil Temperature, deg C. Sheet Thickness, mm kv (max) Time, sec 25 1 30 28 8 8.3 27.2 20.0 25 5 , 54 23 8 94.0 22 1 363.0 20 4 668 18.8 5400 100 1 30 21.0 1.5 20 3 2 19.6 38 18.6 72 170 600 " 15 9 470 15.2 1920 1 25 2 60 52.5 26.0 500 50 47.0 230 25 3 90 80.3 68.0 77.5 130 77.2 350 75.5 1400.0 25 4 1.20 127.2 7.0 120.0 16.0 115.2 45.0 110.0 100 1075 185 105.0 330.0 104.6 730.0 260 DIELECTRIC PHENOMENA TABLE IX. A.c. AND D c. PUNCTURE VOLTAGES OF VARNISHED CAMBRIC FOR VARIOUS THICKNESSES AND TIME OF APPLICATION Time of application, seconds 100 50 10 Sheets Thickness, mm. Kilovolts to puncture (max ) 1 30 a c. 30 d.c. 11 18 16 5 23 5 17 5 24 5 20 5 27 5 25 5 32 5 2 60 a.c. 60 d c. 20.0 43 31 49 5 33 51 39 55.5 47 62 5 3 90 a.c. 90 d.c. 30 70 42 79.0 45 81.0 52 86 62 95 4 1 . 20 a.c. 1.20 d.c. 37 96 52 111 55.0 114 64 123 78 137 Gradient Kv per Mm. (Max.) 1 30a.c. 30d.c. 36 6 60.0 55 75.0 58 5 82.0 68.5 92.0 85 108.0 2 60a.c. 0.60d.e. 33 3 r 72.0 51.5 82.0 55.0 85.0 65.0 92 78.0 104.0 3 90a.c. 0.90d.c. 33.3 77 5 46.5 87.5 50 90 57.9 95.5 69 105.0 4 1 20a.c. 1 20 d.c. 30.9 80.0 43.3 92 5 45.8 95 53.2 102.0 65 106 DATA APPENDIX 261 3. STRENGTH OF AIR FILMS CORONA TESTS ON AIR FILMS BETWEEN Two GLASS PLATES (60 ~. Glass Plate on Each Electrode) Thickness, cm Per- mittivity Corona starting voltage maxi- mum Stiength of air films kv/cm max reduced to 5 = 1 Temp deg C Bai procure 6 Both Air glass cm space plates E 9. " 0025 910 7 2 96 21,100 161 196 285 73 6 0053 910 7 2 96 17,400 137 139 285 73 6 0120 910 7 2 96 10,600 88 95 285 73 6 028 910 7 2 96 9,350 63 59 285 73 6 0562 910 7 2 96 9,050 53 50 6 285 73 6 122 910 7 2 96 10,700 44 5 44 5 285 73 6 275 910 7 2 96 14,300 36 8 39 3 285 73 6 455 910 7 2 96 19,100 35 6 36 8 285 73 6 0051 910 9 3 74 7,660 101 143 114 72 9 0,0122 910 9 3 74 7,050 96 5 95 114 72 9 02(10 910 9 5 73 5,180 58 5 59 6 120 72 9 0560 900 9,4 73 5,890 53,0 50 6 116 72 5 120 900 9 4 73 6,670 42 4 44 4 117 0,275 0,900 9 3 73 10,100 37 3 39 114 72 5 0,455 0,900 9 3 73 14,160 35 1 30 8 110 72 5 Corona on Air Films Between Tape Insulated Conductors 635 630 645 645 3 2 3 5 95 0,75 26,900 33,400 34 36 2 36 1 35 1 25 107 72 8 72 8 (/a strength of entrapped film. * strength of film between metal spheres 800 Dubsky, Dielectric Strength of Air Films Entrapped in Solid Insulation, A I E E , Fob,, 1914. 262 DIELECTRIC PHENOMENA SPARK-OVER OF GAPS AT SMALL SPACINGS AND VARIOUS AIR DENSITIES Spark-over, volts (Max,) f)X So, 010 000132 1050 015 000197 640 020 000264 400 030 000394 355 0.040 000526 350 050 000660 395 100 001320 550 300 003950 700 500 00660 850 700 00920 1030 965 01270 1700 1.930 02540 2200 2 900 03820 2700 3 860 05100 3750 5.800 07650 4680 7 740 1020 5600 660 1270 6530 11 600 0.1520 7370 13 520 0.1770 8210 15 450 0,2010 x = spacing, cm. p = pressure, cm. 5 relative air density. Paschen's Law: To find spark-over voltage multiply pressure or density by spacing and find corresponding J57 m 95.0 100 1.05 8 60 69 5 117.0 1.68 4 25 113.0 117.0 1 . 05 9 85 76 134 1,76 R 430 ohms L - 312 X 10-* honry Q - 0,001 X i(M farads 900 Kilocycles 1 05 9 2 14 2 1 52 0.40 14 1 H.I 1,00 1.20 15.2 28 3 1.86 0.90 28.2 28.2 1 00 1,80 21.0 42 3 1.91 1 40 42 3 42.3 1 . 00 2 00 29 7 50.5 1 92 1.90 55 50.5 1.02 3 10 33.9 70 7 2.08 2.40 08 70 5 1,03 3 60 38 9 84 7 2.18 2.90 82 84 5 1.03 4.00 42.3 99 2.34 3 50 95.0 98 5 1.04 3 70 100 106.0 1.06 R 400 ohms L - 100 X 10-* honrys C - 00025 X l(M farads The above waves are single half cycles of amo waves of the frequency i DATA APPENDIX 265 Bar * 76 cm Corona TABLE III. TRANSIENT CORONA (Single Half Sine Wave) Concentric Cylinders in Air t = 25 deg C 5 1 Outer Cyl. rad. R = 8 8 cm Wire radius r cm 60 ~ tests Impulse tests Calc corona kv. (max ) Test corona kv. (max ) Test spark- over kv (max ) Corona Spark- over kv (max.) lin 10 Single half sine wave frequency kilocycles A kv. (max ) B kv (max ) 0318 13 4 135 13 8 14 7 15 1 15 6 16 16 1 100 100 500 900 0573 20 5 20 110 21 2 22.0 22 6 23 7 24 24 100 100 500 900 130 31 4 31 3 49 6 32 3 33 5 34 2 33 2 34 34.8 103 100 500 900 95 86 85 86.0 85 87 87 5 86 87 5 88 108 100 500 900 1 425 100 98.0 98.0 99 99 100 99 99 5 101.0 110 100 500 900 Bar 70 cm I 25 deg C R a 3 81 cm 0^0129 5.7 .. . 8 5 9 2 9 5 . .. 32 68 100 500 900 0318 12.3 12.0 49.0 13 4 13 5 14 5 14 7 14 7 15 33 67 5 100 500 900 0573 17.2 .... 40 17 4 20.0 24 18 2 20 5 24 7 35 66 100 500 900 239 33.5 .... 33.9 33 4 87.0 37.1 38.9 37 44 7 63 7 103.0 100 500 900 318 38.0 37.9 37 9 38,5 39.5 41 6 39.0 40 42.0 45 64 98 100 500 900 0.035 49.0 48 1 48.1 49,0 50 51 6 49 7 50 5 52.0 50 62.0 81 100 500 900 1.27 55.0 55 54 5 55 56 56.0 55.0 56.0 56.0 55 57 59 3 100 500 900 Comparison of 60 ~ and transient corona for different sizes of wire in center of a cylinder The voltage at which transient corona first appeared ie given in col. A, Corona appeared on ovory application for voltages Riven in col. B. The difference is probably for positive and negative wire. 266 DIELECTRIC PHENOMENA Air Density TABLE IV. EFFECT OF AIR DENSITY ON TRANSIENT CORONA AND SPABK- OVER Concentric Cylinders 1 Outer cylinder radius, R = 3 08. Inner cylinder, i = 0573 cm Corona, Spark-over Single Meas. 60 ~ kv. Cal. eo~ kv. Impulse kv. max. Impulse ratio 8 60 ~ kv max Impulse kv max Impulse ratio half sine freq. max max kilo- cycles 2 8 2 75 3 5 1.27 064 10.7 064 100 4,8 4 80 5 5 1 15 160 7.0 13 1.86 160 100 6 5 95 6 65 1.13 0.248 9 3 15,5 1 67 0,248 100 7.6 7 57 8,4 1.10 0.330 11 17 5 1 59 0.330 100 11.6 11 60 12 7 1 09 0.630 16 6 27 3 1 05 630 100 14 4 14.40 15.5 1.07 847 20 2 30 2 1 50 847 100 16 2 16 20 17.2 1.06 1.00 22 5 31.9 1.42 1.000 100 2.6 2 58 4 1.55 0.051 28.5 0,040 900 4.8 4,86 6.5 1.34 0.166 5 31.0 6.2 085 900 7.6 7 60 10.1 1.32 0.333 7 5 37 4 94 0,173 900 9 5 9,50 12 1 1.28 465 13.3 47.0 3 54 0.440 900 13.5 13 30 16.3 1 23 0.765 15 8 53.0 3 35 , 590 900 16.2 16 20 20.0 1.23 1.00 18 8 60 3.10 0.765 900 22 K 7 K 2 (M\ 1 rtA AAA Outer Cylinder Radius, R 3.08 cm. Inner Cylinder, r m 0.635 cm u\/v 7.3 7 7 8 5 1.16 0,127 7.3 8.5 1,16 127 100 13.0 13 14.9 1 14 0.253 13 14 9 1 14 0.253 100 15 15 3 16.6 1.11 0.309 15.0 16,6 1.11 0,309 100 17 16 8 18 3 1.08 350 17 18,3 1.08 0.350 100 24.0 23.8 24 5 1.02 0.535 24.0 24 5 1.02 0.535 100 29 29.0 28 9 1.00 0.702 29,0 28,9 1,00 702 100 34,5 35 5 34 5 1.00 863 34.5 34.5 1,00 0,803 100 39 40,3 40 5 1.03 1.002 39.0 40.5 1.03 1,002 100 Outer Cylinder Radius, R m 3 08 cm. Inner Cylinder, r * 0,635 cm 3.5 3 9 8 6 2 46 0.049 3.5 20,3 5.80 0.040 900 9 9,8 11 9 1 31 165 9,0 25.0 2.78 0,165 900 14 14 I 17 3 1.23 0,280 14.0 30 5 2.18 280 900 21.2 21,2 22 5 1.07 0.462 21 3 37,6 1 77 462 900 26.2 26 3 28.0 1.06 0.604 26 43,6 1,67 0,004 900 32 32.2 35.6 1.01 0,773 32 48.5 1.52 0.773 900 39.0 40.3 40.2 1.00 1.00 39.0 52.5 1.34 1.00 900 1 Tests above made in a metal lined ftlaas tube. DATA APPENDIX 267 Polarity TABLE V. POSITIVE AND NEGATIVE SPARK-OVER (Dissimilar Electrodes) Wire in Cylinder R = 3.81 cm Radius, cm Voltage kv Per cent, difference wire 4- - 1.27 187 0318 57 51 49 8 57 58 5 60 6 15 22 Point and plate Spacing cm. for a given applied voltage when point is 5 15 3 05 Approx. 500 kilocycle wave Air Films TABLE VI. TRANSIENT SPARK-OVER VOLTAGES AT SMALL SPACINGS (Between 6 25 cm. Diameter Spheres 5 = 1) co~ 100 kc. impulse 900 kc impulse Spark-over Spacing, Gradi- Gradi- Gradi- cm. Volts max. ent max. Volts kv. ent kv. por Impulse ratio Volts kv. ent kv per Impulse ratio kv kv. per cm cm cm 0025 50 196 78 305 1 57 81 325 1 64 0.0051 0.73 143 1.23 242 1 69 1 10 216.0 1.51 0.0076 0.90 118 1.70 212.0 1 80 1 78 235 1 98 0.0102 1,07 105 2.11 207.0 1.98 2 18 215 2 04 0.0127 1,17 92 2.44 192.0 2,08 2 55 200 2.18 0,025 1,52 60 4,50 178.0 2,95 5 00 198 3 04 0.051 2 62 52 6 15 122 2 35 8,50 168 3.25 102 4,62 46 8 75 87.0 1 90 12,80 126.0 2 77 0.25 9.77 40 14.90 61 1 52 21 50 84,1 2.20 0,51 17,50 36 22.50 46 1 28 28.50 56 1 63 1 27 39 20 35 42 00 37.0 1,06 47 00 37 1 20 1.90 57 50 35 57,50 35 1.00 62.50 36 1 09 2,54 88 50 35 88.50 35.0 1 00 90 00 35 1 02 Accuracy of im pulse voltages bot above 5 kv. 268 DIELECTRIC PHENOMENA Insulators TABLE VII. EFFECT OF POLARITY ON INSULATOR SPARK-OVERS 200 kc 60 ~ spark- over kv , ma^c Impulse spark-over kv varying polarity, max. Impulse spaik-over kv predetermined polarity, max Cap + Cap 98 1 spark-over in 10 impulses. 108 108 10 spark-overs m 10 impulses. 130 134 TABLE VIII. IMPULSE SPARK-OVER OF SUSPENSION INSULATORS WET AND DRY Ins No Type 60 "-' arc-over (max ) 100 kc. impulse 500 kc impulse arc-over arc-over Dry "Wet Dry Wet Dry Wet A Two piece suspen- sion, with petti- coats 112 72 118 114 165 162 B Two piece suspen- sion with petti- coats. 116 70 128 125 172 168 DATA APPENDIX 269 TABLE IX SPARK-OVER VOLTAGE OF INSULATOR AT DIFFERENT AIR PRESSURES DURING RAIN (Sec Fig. 96) Kain Tests (0 2 in. per Minute at 45 deg ) Room bar. cm Vacuum cm (in the cask) Pressure crn (in the cask) Temp c (in the cask) 5 (in the cask) Kilovolts spark-over (effective) 60-cycle Spark-over 75 6 41 2 34 4 18 46 28 75 6 36 39 6 18 53 31 75 6 31 1 45 5 18 61 35 75 6 25 50 6 18 68 39 75 6 15 6 59 18 79 45 75 6 7 8 67 8 18 91 50 75 6 75 6 18 1 02 57 Impulse Spaik-over 200 Kilo Cycles Single Wave (Effective Kv.) 75 6 41 2 34 4 18 46 62 75 6 36 39 6 18 53 68 75 6 31 1 45 5 18 61 72 75 6 25 50 6 18 68 77 75 6 15 6 59 18 79 84 75 6 7 8 67 8 18 91 92 75,6 75,6 18 1 02 98 F. W. Peek, Jr , " The Effect of Altitude on the Spark-over Voltage of Bushings, Leads and Insulators," A I.E.E., Dec , 1914. G. E. Review, June, 1916. Tests made in a large wooden cask. 270 DIELECTRIC PHENOMENA Oil TABLE X. IMPULSE AND 60 ~ BREAK-DOWN VOLTAGES IN OIL Spacing, cm 60 ~ kv max Impulse kv max Impulse ratio oil Impulse ratio same spacing in air / Between Disks 2.5 cm. Diameter 5 56,6 170 3 00 Approx. 230 kc. Between Needles 1 50 103 2 00 .... 2 69.0 157 2,20 1.20 Approx. 230 kc. 3 89.0 233 2.60 1.21 4 108.0 321 3.00 1 25 2 T 54 Spheres Small Spacings Spacing less than 4 \/R 0.25 70 160 2.30 50 100 245 2.45 Approx. 230 kc. 0,70 115 270 2.35 1 00 140.0 285 2.05 TABLE X (Continued).- -IMPULSE AND 60 <~~ BEEAK-DOWN VOLTAGES IN OIL Between 2/0 Needles Needle spacing, cm. 60 ~ spark- over kv, (max.) Impulse, kv. Impulse ratio / 0.32 28.0 36.5 1.30 100 kc. 64 1.27 40.0 63,0 70.0 128.5 1.75 2.04 (single half sine 1.70 2 00 74.0 81,0 175.0 2.37 wave) 3 00 104.0 0.20 20 36.0 1 80 500 kc. 32 0.42 28.0 31.5 64,0 92.0 2.30 2,92 (single half sine 0.56 37.0 121.5 3.29 (wave) DATA APPENDIX 271 TABLE XL COMPARATIVE STRENGTH OF OIL FOR HIGH FREQUENCY, IM- PULSE, OSCILLATORY, AND 60 CYCLE VOLTAGES (Transil Oil Between Flat Disk Terminals, Square Edges. 2.5 cm. Diameter ; 25 cm. Space) Break-down Gradients 60 cycle kv per cm. max Single impulse sine shape corresponding to 200 kilocycles, kv per cm max. Damped oscillations train frequency 120 per second. Fre- quency 200 kilocycles, kv. per cm max. High-frequency al- ternator 90 kilo- cycles, kv. per cm max 170 390 300 67 Solid Insulations TABLE XII. COMPARATIVE INSULATION STRENGTH POR HIGH FREQUENCY, IMPULSE, OSCILLATORY AND 60 CYCLE VOLTAGES Temperature 30 deg. C. 60 cycles High frequency (alternator) 90,000 cycles Damped oscilla- tion. Train freq 120 sec. 200,000 cycles Single im- pulse sine shape, cor- responding to half cycle of Imp ratio Thick- ness, cm. Lay- ers 200,000 cy. kv. per cm. kv. per cm. kv. per cm kv per cm. (max.) (max.) (max) (max ) Bapidly applied 1 mm. Rapidly applied 1 mm Rapidly applied 1 min Bapidly applied 1 mm. Rapidly applied 1 mm Rapidly applied 1 min Transil Oil Between Mat Terminals Square Edge 2 5 cm Diameter 25 cm Space i 170 67 300 390 2 10 0.25 1 0^hd Presaboard 10 cm. Diameter Square Edge Disks in Oil 355 395 310 370 95 61 25 72 41 17,6 370 420 290 240 720 2.3 0.25 50 1.50 1 2 3 Varnished Cloth 10 cm. Diameter Square Edge Disks in Oil 530 465 195 176.0 1080 2,26 0.06 2 420 310 135 100.0 550 560 780 2 50 15 5 420 310 100 73.0 490 410 700 2 25 0.25 8 830 275 410 305 600 2.20 36 12 "Rapidly applied" voltage brought to puncture value iu a few seconds 272 DIELECTRIC PHENOMENA d. STRENGTH OF OIL AT LARGE SPACINGS BETWEEN POINTS Spacing, cm. Spaik-ovei , k v max. 5 * 127 10 226 20 395 30 510 40 610 50 662 60 735 70 805 FLAT Discs WITH ROUNDED EDGE 25 cm. diameter Radius of edges, 2 5 cm. 5 310 10 460 15 650 20 780 25 900 If the space between the discs is divided into ducts by press- board barriers, the total breakdown voltage will be increased. Incipient sparks will, however, start at the voltages in the table. It is assumed that the barriers do not occupy more than 25 per cent, of the space. The above tests were made on dry oil at 60 cycles. INDEX PAGE Air, at veiy low pleasures ... . . 196 compressed 42 density . 51 occluded in solid insulation 236 see Corona. Altitude, effect of, on arc-over of bushings, leads and insulators . Ill, 217 effect of, on corona 42, 50, 51 effect of, on corona loss . 146 effect of, on sphere-gap spark-ovei . 95 variation of air density with . 51 B Barriers in oil appendix, 1,55, 169, 189, 272 Beta particle 193 Bushing, condenser type . 220 effect of altitude on spark-over of 111 oil-filled type, . . 220 ovorstroHsod air in ... ,217 rod and torus . , . . , . 220 transformer ..... ... , 220 C Cable, graded . . 33, 218 Capacity, aeo Permittance Cathode rays .. ... . 192 Compressed air , , 42 Corona, application of electron theory to . , , * 194 at very low air density. . . - . 196 calculations for practical transmission lines ... . 199 condition for npatk or. . . . . 27, 79, 84 in entrapped air films . , . . . appendix, 61, 196, 236 m oil . . . 155 Corona loss, a.c. and d.c. . . , . ... ... 132 description of experimental lines . . . 117 disruptive critical voltage. . . . , . , . 137 273 INDEX PAGE Corona loss, effect of frequency 129 effect of humidity, initial lonization, etc 147, 148 effect of moisture, frost, fog, sleet, rain and snow. . 145, 149 effect of smoke and wind . . 149 effect of temperature and barometric pressure 146 for small conductors 136, 137, 140, 142 harmonics due to . ... 118, 207 law of , . 134, 137, 140, 142 loss near the disruptive critical voltage .... .143 probability law . . . 148, 152 quadratic law j 121 Corona, on generator coils 216 Corona on transmission lines, see Transmission lines. Corona, visual, a.c. and d.c appendix, 38, 42, 44, 52, 75 application of electron theory to. . . 41, 47, 194 calculation for concentric cylinder 48, 53, 57, 63 calculation of gradient 40, 42, 47, 53, 63, 67, 71 calculation of voltage . 43, 54, 57 calculation of voltage wet.. . 67,237 derivation of law of .... 49, 53, 63 diameter of 74, 78 effect of air density 42, 51 effect of barometric pressure 50 effect of cables 43,71 effect of conductor material 43, 44, 46, 48, 68 effect of conductor surface. . , ......... 43 effect of current in conductor 43, 68 effect of diameter of conductor 39, 44, 46, 48 effect of dirt 66 effect of humidity 43, 68 effect of initial ionization 43, 68 effect of oil 43,66 effect of small spacing 42, 57 effect of spacing .... , 39, 44, 45, 46 effect of temperature on , 50, 51 effect of water on 43, 66, 67 effect of wave shape. ... 43, 6-5 in C0 2 and H influence of frequency on , 65 on conductors of same potential close together 71 law of, for concentric cylinder 48, 53, 57, 63 law of, for parallel wires 40, 42, 43, 54, 57, 63 mechanical vibrations due to ..,.,... 78 photographic study of 73 positive and negative *.,...... 75 rectifier 76 stroboscopic study of . * 73 transient appendix, 108 INDEX 275 PAGE Cylinders, concentric, flux density. ... . 13 gradient .13,29 permittance or capacity . 13, 29 visual corona, see Visual corona. . 38, et seq. spark-over and corona in oil ... . . 159 parallel, see Wires. D Dielectric, addition of fluxes . s . . ... 14 circuit .,.'.. 215 displacement. . ... 9 flux control 35, 223 flux density between concentric cylinders 13 flux density between parallel planes 11 flux density for parallel wires 14, 23 flux densities, sum of at a point 16, 20 flux refraction 30 formulae for different electrpdes 29 hysteresis 36, 37 spark lag in air 108 spark lag in oil 162 spark lag in solids 117 Dielectric field, analogy with Hooke's Law 4, 9 analogy with magnetic field 2 between concentric cylinders .... 12, 33 between parallel planes 10 between parallel wires 14 control 223 energy stored in 8, 9, 10 energy transfer in transmission 8, 9, 10 equation of equipotential surfaces between parallel wires, . . 16 equation of equipotential surfaces for spheres 25 equation of lines of force between parallel wires 20 equation of lines of force from spheres ... 25 experimental determination of 2, 232 image of 234 in, three dimensions 232 methods of constructing 226 resultant 14 superposition of ....,..., 14 three phase. 238 Dielectrics, combination of dielectrics of different permittivities 30 combination of, in multiple 34 combination of, in series 31 gaseous 38,79,117 liquid.,... 153 solid 166 276 INDEX E PAGE Elastance, ..... ' . .11, 215 Elastivity . 11, 215 Electron theory application of, to visual corona 41, 47, 194 general discussion of 192 practical application of 194 Energy distance 41, 42, 48, 57, 156, 195 Equipotential surfaces, construction of 226 equation of, for paiallcl wnes 16 equation of, for sphcies 25 in three dimensions 232 Experimental study of, corona loss. . .117 dielectric fields 2, 232 solid insulations 166 spark-over . 79 strength of oil . .153 visual corona . 44 p Flux, see Dielectric flux. Frequency, effect on corona loss . . 129, 1,52 effect on visual coiona. 65 see High frequency. G Gamma rays . , . , .... 193 Gap, method of measuring high voltages . 87 needle , , 87 sphere. , 88 Green's theorem . . .22 Gradient, at any point . . . . , , , , . 21, 23, 230 at different points around a comluotoi 231 between concentric cylinders , 13, 29 between largo spheres ... . .... 26 between parallel plancw. . , , 29 between parallel wires. . , . 23, 26 equigradient surfaces 231, 232 law of visual corona, see Visual co ion a . ., 38 ct seq. Guard rings 223 ir Harmonics clue to corona . . . . . , 118, 207 High frequency, effect of, in design . 177, 225 effect of, on corona los l% INDEX 277 PAGE High frequency, effect of, on oil, . 165, 184 effect of , on solid insulation . . . . 177,184,187 effect of, on spark-over of sphere gaps . 105, 106 loss in solid insulation . 187 Hysteresis, dielectric , 36, 37, 166, 185 Images . 234 Impulse ratio . , 108 Impulse voltages, effect of, on air . 108 effect of, on spark-over in oil 162, 165, 187 effect of, on solid insulations 177, 184, 187 measurement of . . . 108 Insulation, breakdown caused by the addition of . 213 Insulation, breakdown, how measured. . . 12 Insulation, solid, area of electrode. . . .... 175 barriers in oil ... . . 189 breakdown caused by addition of . .213 common . 1 56 comparison of breakdown in oil and m air. . . 170 et seq. comparison of strengths for impulses, oscillations, high frequency and low frequency 184 cumulative effect of overvoltages of short duration . 178 d,c strength ... . appendix, 191 effect of d.c. on 191 effect of impulse voltages and high frequency on . . . 177, 184, 187 energy loss in . . . . 185 high frequency loss in ... . 187 hysteresis 166 impregnation of 190 laminated . 175 law of energy loss in 185, 187 law of strength vs. thicknenH . 174, 237 law of strength vs. time . . 178 mechanical 190 methods of testing 170 et seq. occluded air in 61, 191, 196, 236 operating tompcraturoH of . , . 188 permittivity of 179 resistance 37, 167 strength under high frequency 184 strength under impulses 177, 184 strength under oscillations 184 strength vs. thickness 174 strength vs. time 178 tables of properties of ISO, 184 278 INDEX PAGE Insulations, air . .38,79,117 compressed air . 42 gaseous . 38, 79, 117 liquid ... 183 oil. 183 solid 166 Insulators, effect of altitude on spark -over ol .111 Lead, see Bushing. Lines of force, construction of. . , , , ... .... 226 equation of, between parallel wires . . 18 equation of, for spheres 25 equation of, three-dimension field , ... 232 perpendicular to equipotential surface , . 20 Liquid insulations, see Oil. M Magnetic field, analogy with dielectiic field 2 experimental plot of . , 2 N Needle gap 87 effect of humidity on . . . 88 spark-over in oil . . . , 154, 156 spark-over voltage in ram 105 Oil, barriers in 161,189 corona in 155 corona and spark-over in 153 d.c. strength ... , appendix, 165 effect of moisture in 154 effect of temperature on 155 formulas for strength of . , 159, 161 high frequency in 165 law of spark-over and corona, , . , 159, 161 needle gap spark-over in 156 permittivity of . . 155 physical characteristics of trantdl oil , . 153 spark-over for different electrodes m , , . . , . , ,.,154 specific resistance in ... 155 surface leakage in 188 transient voltages in 102, 184 INDEX 279 PAGE Oscillations, effect of, on solid insulations 177, 184 effect of, on sphere-gap voltages .105 measurements of 105, i08 P Paschen's Law 196 Permittance or capacity, between concentric cylinders . . 13, 29 between concentric spheres 25 Permittance or capacity, between eccentric spheres ... . . .29 between parallel planes . 10, 29 between parallel wires ... , . 22 : 29 comparison of single phase and three phase 235 effect of ground on for parallel wires 223 formulae for different electrodes . 29 in. series . . , 12 Permittivity . . ... 11 of oil . 155 of solid insulations ... 179 Planes, parallel, flux density. . , .... ..10,11 gradient. . ... 10 permittance or capacity of . . 10 spark-over in oil . . .157 Potential at a point ... ... , 14 Potential difference between two points ... .... 14 Potentials, addition of ... 14 Problems, breakdown caused by addition of stronger insulation . 213 bushing . . 220 condenser bushing . . . 220 dielectric field construction of , . 226 dielectric field control. . 223 dielectric field experimental determination of , . , . 232 dielectric field in three dimensions 232 effect of ground on dielectric field between parallel wires . 234 entrance bushings 217 general problems on the calculation of spark-over of parallel wires, insulation loss, strength, etc 236 graded cable . . 218 high frequency .^ 225 static, on generator coils 216 three-phase dielectric field for flat and triangular spacings . 234 S Spark-over, at small spacings appendix, 63, 93, 196 condition for .spark or corona 27, 79, 84 d.o. , appendix, 107 effect of altitude on, for bushings, insulators ........ Ill, 217 280 INDEX PAGE Spark-over, effect of altitude on, for spheres . . . . , 95 effect of water and ram on . 105 for needle gap .... . . 87 for parallel wires 79 for spheres 88 gaps used in measuring high voltage . ... 87, 88 influence of water and oil on 86 in oil . . . . . 186 ram and wet on insulators . . appendix, 116 lightning and transient , appendix, 108, 116 Specific resistance, of oil 155 of solid insulation 167 Spheres, air films between , . . .58 as a means of measuring high voltage . 88, 101, 103, 104 concentric permittance, dielectric field 25 corona or spark-over for . . , 58 density correction for air films , . appendix, 61, 196 effect of ground on spark-over voltages . 104 effect of water and rain on arc-over voltages 105 experimental determination of effect of altitude 95 law of disruption , 63 law of spark-over in air 63 law of spark-over in oil 159, 161 precautions against oscillations 101 rupturing gradients for different si^cs 62 spark-over at high frequency, oscillations and impulses 108 spark-over calculation of . . 92, 93 spark-over calculation of, correction for altitude 93 spark-over curves 89 et seq* spark-over curves at small spacings 60 strength of oil around . 161 two large equal spheres, field between gradient, permittance, etc 25 two small equal spheres. . 28 Steep wave front 105, 108, 162, 177, 184, 187 Surface leakage, air 189,190,221 oil 188 Symbols, table of xiii T Testing, method of testing solid insulations 170 et. seq. Third harmonic 118,207 Three-phase dielectric fields between conductors with fiat and triangu- lar spacings 238 Transformer, bushing . 232 condenser bushing 220 oil-filled bushing , 232 INDEX 281 PAGE Transformer, voltage rise due to high frequency testing. 225 voltage rise due to spark-over . ... .102 Transmission lines, agreement of calculates and measured corona losses 208 corona limit of voltage on, with, working tables. . .210 corona on 199 practical example of corona loss calculation 205 practical formulae and their application 203 practical method of increasing size of conductors. 207 safe and economical voltages 207 three-phase, comparison of permittance with single- phase . ... 234 three-phase, with triangular and flat spacing . 234, 235 spark-over voltage of. ... .... 83, 237 voltage change along lines . . . 208 U Units, table of . . , , , . . xi v Visual corona, see Corona. W Weather, effect of, on corona loss ' 145, 146, 149 Wires, calculation of spark-over on, wet and dry . 237 calculation of visual corona-on, wet and dry . 237 corona loss on . 117, 199, 238 effect of ground on permittance or capacity and gradient ... . 233 equation of cquipotential surfaces , , 14, 16 equation of lines of force . 18 experimental plot of field between 2, 232 flux density 14 gradient 23,29 law of spark-over and corona in oil . , ..,159 lines of force 14 method of drawing dielectric field for , * 226 permittance or capacity , 22, 29 spark-over 79 spark-over, wet > 96 visual corona, see Visual corona, . . . 38 et seq. X 3 SHfiE DDMDH 3365 1 1987 621.3156 P36 c.2 Peek, Frank William, Dielectric phenomena in high voltage engineering University Libraries Carnegie-Mellon University Pittsburgh, Pennsylvania 15213 DeaddlfJed using th Bookkeeper process Neutralizing Agent Magnesium Oxid Treatment Date j- j- Q II