book
Dielectric Phenomena in High Voltage Engineering (1915) — part 11 of 12
1 January 1915
'
■
8.63
6.73
5.83
5.40
5.29
1 Such a gradient does not e
iat on this line and hence Z] is imaginary.
(See plot F
g-8,f
«iiel6.)
Gradient at Equidistant Points on the Conductor Surface
Ancls iMt. horiHinUl a',A'>\ ud Un« throuch polot ud 0*
30"
eo*
BO"
120°
IW
180"
26.7
26.0
23.7
21.6
19.4
18.2
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 Xs 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 16. 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 in 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 ceUs.
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
— = constant.
z •
This can readily be seen from Figl 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.
CONSIDERATION IN THE DESIGN OF APPARATUS 233
ftl
M\
JUaf
Bod
\5
it is thus possible, without great difficulty, to draw a field by a series of approximations in which the cells have a constant
- or add up to maximum permittance. 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.^ 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.
^ 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.
Solid Gel Formed
by Botatlni Plane OeU «bo«««
Fia. 189.— Dielectric field three dimensions.
in
234 DIELECTRIC PHENOMENA
Voltages between AB due A, By Ai^ Bi are
*^ - + ^2^^ ^^8. f
«B
~ ^2wkK^ ^°^ S /S a S' where the wires \ _ ( ^ -) in„ ^ \ are far apart. /
e = ex +fiB + «A. + «B. = ;^ (logf + log. ^) - ;^ logf
The total voltage b
S . , 2A\ ^ , S2A
r a
^ = f = i^ (««*• "°^)
r a Where the wires are far apart the gradient is
e
^"o 1 S 2h
2 r log. — —
^ r a
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 ^ ^ ' ^f difficult as a number of simul-
^ n taneous equations must be writ-
I \ / 1 ten and solved,
t \ / 1 Case 12. Three-phase Di-
I \ / electric Field with Symmetrical
^»^iM mM^M ^"^'^ andUnsymmetricalSpacings.—
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
17,^ 1AA T?4r » f , above. The effective or maxi-
FiG. 190. — ^Effect of ground on ca- 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 I C
1 AB r CB
(a) EjiB = 2^j^ (^^ ^^^ T" + ^^^^^BA + ^c log. ^) =e sin ^
6 sin (^ - 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 + ^c =
A o
Conductors SpcLced in a Triangle o o (equilateral triangle).
B C Substituting spacing S in (a) and (6) and solving for ^^^ ^q, and ^^
2irkKe ^^ = o (1.5 sin e + 0.866 cos 6)
Slog.- r
Let c(1.5 sin 6 + 0.866 cos 6) = «« (sin ^ — a)
put ^ = 90 and ^ = and solve for €„ and a
2TrkKe . ,^ ,.^. 1.16(^fciiL)e . ,^ _.. ^fl = osm {$ - 150) = g ^ sin(^ — 150)
Vsiog*- log.-
2irAiiLe . ,^ ^^. 1.16(7rfcii:)e . ,^ ^^ ' ^^ = o sm {e — 30) = ^ g sm (^-30)
VSlog.- %.-
^(7 may be found in the same way, or for this particular case, ^A9 4^bj *^d }pc are equal by symmetry. For single phase:
2'KkKe
2hg.^
Therefore, when the wires are far apart, and with the same voltage between lines, the three-phase stress is —7= times the single-phase stress.
236 DIELECTRIC PHENOMENA
Flat Spacing A B C. — Putting S, 5, and 2S ia a and b and
o o o
solving as before,
^B = z sin ie - 150)
VS log. - - 0.58 log 2 r
^kKe . , _^,
= ^^ sin {$ - 150)
V3 log. ^ - 0.4
The flux, and therefore the stress, when the wires are far apart,
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 ^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 spacings.
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 paraUel 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. It is probable that the solid 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^ from the formula on page 67, Chapter III. Insert the value in formula (20). Maximum e, to neutral is thus found. If the voltage used is a sine wave, reduce to effective kv. by dividing by y/2. For a three-phase line the voltage between wires may be found by multiplying by /3; 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 5 « 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 1/120000 second? In 100 seconds?
Use equation on page 179, Chapter VII, of the form
9m = 1/(1 + T^) ^» "^ g» 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?
0.94,
, = 7.5(i+:^y)
where t = thickness in mm.
g = gradient in kv./mm. (eff.)
(See Chapter VII, page 174.)
DATA APPENDIX
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.
Corona Loss — Indoor Line — 60-cycle
Test lOB
Test IIB
Eff. kv. to neutral, e*
Amp. per km.
LOM
kw./km., p
Eff. kv. to neutral, tu
Amp. per km.
Loes kw./km., p
10.52
0.07 0.51 1.40 3.20
4.02
6.83
9.44
15.03
20.63
13.7 16.7 18.1 19.9
24.7 29.3 33.2 36.3
39.7 44.0 47.3 60.2
45.2 41.5 37.4 31.0
27.0 22.3
0.33
12.62
0.92
14.80
1.11
17.10
0.070
0.100 0.160 0.189 0.223
0.268 0.325 0.380
1.64
18.20
3.95
19.60
6.90
22.30 24.90
27.20 29.70
0.225 0.310
0.395
10.40 14.20
18.75 26.73
28.00 25.90
0.404 0.342
0.263
22.40 16.80
11.80 7.16 4.14 1.98
34.20
23.60 20.80
0.350 0.293 0.238 0.163
0.128 0.082
29.20 22.20
18.40
15.69
16.10
8.08
6.29 2.53
Spacing, 15.25 cm.
Radius, 0.032 cm.
Total cond. length, 0.0838 km.
6 - 1.02.
Spacing, 30.5 cm.
Radius, 0.032 cm.
Total cond. length, 0.0838 km.
8 - 1.02.
238
DATA APPENDIX
239
Tert 13B
•
Test 15B
Eff. ky. to neutnl. e*
Amp. per km.
kw./km., p
Eff. kv. to neutral, en
Amp. per km.
Lo« kw./km., p
19.5 24.3 29.6 34.0
38.0
0.051 0.071 0.099 0.133
0.146
0.96 1.78 3.23 4.95
6.49
9.13 12.51 16.35
21.00 26.25 34.40 40.60
1
50.50 59.50 72.00 83.10
93.40
17.3
23.7 30.2 36.1
42.2 49.8 56.7 62.5
66.5 71.4 78.6 84.4
89.4 95.4 99.3 91.0
81.6 67.9 52.1 39.1
27.0
0.059 0.078 0.109
0.35 1.17 2.34 3.92
5.76
43.0
0.166 0.200 0.223
0.246
9.26
46.7 62.4 .
57.5
0.196 0.224
13.21 16.70
20.00
62.5
0.285 0.327 0.359
0.385
24.35
68.3 73.1
79.1 84.0
0.310 0.322
0.345
30.95 37.20
41.90 50.50
90.0 93.6]
102.0
0.430 0.460
0.510
0.395 0.369
0.310
58.60 45.60
34.10 21.65
0.177 0.126
0.068
10.46 4.44
1.74
Spacing, 61 cm^
Radius, 0.032 cm.
Total cond. length, 0.0838 km.
9 -> 1.03.
Spacing, 91.5 cm.
Radius, 0.032 cm.
Total cond. length, 0.0838 km.
« - 1.012.
240
DIELECTRIC PHENOMENA
Spacing, 122 cm.
Radius, 0.032 cm.
Total cond. length, 0.0421 km.
5 -> 1.018.
Te8t20S
Test 21B
EflF. kv. to neutral, e*
Amp. per km.
Lon
kw./km., p
1
Eff. kv. to neutral, e%
Amp. per km.
Loaa
kw./km., p
17.8
0.21 1.29 2.17 3.71
5.16
6.94
9.80
14.60
19.23 21.12 26.70 33.10
42.70 61.70 35.60 25.00
15.95 7.44 4.55
19.8 24.5 27.2 30.7
34.8 39.8 44.8 50.4
55.1 60.6 64.6 70.0
77.9
87.6
94.3
101.6
1
0.81
24.6
1.15
30.1
. 2.02
36.2
0.110
0.128 0.159 0.190 0.233
0.258 0.273
2.19
42.0
3.42
47.0 63.2 62.0
67.6 73.4 78.1
0.129 0.156 0.177
0.212 0.234 0.246 0.266
0.310
3.86 6.04 6.47
8.45 10.80 12.40
85.2
93.2 100.2
0.346 0.385
15.10
19.30 26.60
87.0
0.350 0.298
0.250 0.178 0.114
32.60
76.1
41.00
66.2 49.4 40.1
k
Spacing, 183 cm.
Radius, 0.032 cm.
Total cond. length, 0.0342 km.
« = 1.012.
DATA APPENDIX
241
Test 22B
Te8t24B
Eff. kv. to neutral, en
Amp. per km.
Lon
kw./km., p
Eff. kv. to neutral, e*
Amp. per km.
Loas kw./km., p
20.7
0.72 1.01 1.21 1.98
2.34
3.57 ;
4.53 1 5.71
7.43
9.13 11.05 11.99
16.37 23.00 26.00 34.50
20.1 25.3 32.0 36.0
41.0 45.7 50.3 57.0
62.2 67.3 72.4 77.5
82.3 87.8 92.5 97.3
100.5 79.0 65.0 52.7
0.24
24.5
0.98
27.2
1.84
30.9
0.103
0.120 0.138
3.18
34.6 40.1 45.2
0.100 0.121 0.149 0.171
4.52 6.11 8.30
50.3 55.1
0.185
0.210 0.240 0.266 0.290
11.57 15.10
60.2 64.6 69.5
0.215 0.230
19.15 23.20 27.50
78.5
32.10
87.5
0.345 0.380 0.417
37.90
94.2
43.80
103.2
50.80
55.60
28.70
17.10
9.90
Spacing, 274.5 cm. Radius, 0.032 cm. Total cond. length, 0.0342 km. 2 = 1.012.
Spacing, 91.5 cm.
Radius, 0.057 cm.
Total cond. length, 0.0818 km.
8 » 1.0009.
242
DIELECTRIC PHENOMENA
Te8t26S
Teet28B
Eff. ky. to neutral, «»
Amp. per km.
LOM
kw./km., p
Eff. kv. to neutral, em
Amp. per km.
Loes kw./km., p
20.0
0.37 0.98 2.24 3.36
5.14
6.60
9.90
12.32
18.30 22.30 28.40 36.60
40.80 50.50 56.50 64.00
71.40
83.40
104.00
54.50
39.00 33.00 22.70
10.6
14.2 16.1 18.4
20.2 22.2 24.0 25.0
27.0 30.2 34.0 36.7
36.7 40.7 44.5 47.1
51.7 49.6 43.0
23 2
0.053
29
0.18
32.8
0.43
37.1
0.124 0.141 0.173 0.202
0.232 0.262 0.290 0.332
0.334
0.413 0.431
0.464 0.515 0.562 0.396
0.333
0.98
41.1 46.7 51.3
57.1 61.1 66.2 72.0
75.7 80.7 85.0
88.7
91.0
96.5
101.0
82.8
74.7 69.7
0.061 0.069 0.072
0.087 0.120 0.157 0.178
0.181 0.212 0.265 0.298
0.369 0.342 0.251
1.34 1.83 2.20
2.93
5.00
7.88
10.30
10.10 14.80 20.30 24.80
35.20 30.80 18.20
60.0
0.255
Spacing, 0.61 cm.
Radius, 0.057 cm.
Total cond. length, 0.08186 km.
8 - 1.002.
Spacing, 30.5 cm.
Radius, 0.057 cm.
Total cond. length, 0.0818 km.
a " 0.993.
DATA APPENDIX
243
Eff. kv. io neutral, ««
TestaOB
Amp. per km.
Teet 32B
kw./km., p
Eff. kv. to neutral, ««
Amp. per km.
Spacingi 61 cm.
Radius, 0.071 cm.
Total cond. length, 0.0815 km.
d - 0.98.
kw./km., p
21.7
0.18
0.92
. 2.45
22.5 27.2 32.5 37.2
41.1 45.6 50.3 55.0
60.0 65.7 72.0 77.2
82.5 89.2 92.2 85.2
70.0 61.7
0.21
25.6
0.049 0.062 0.086
0.100 0.123 0.146 0.178
0.194 0.222 0.257 0.278
0.298
0.31
31.5
1.41
36.2
4.30
5.80
8.60
11.70
15.30
19.50 24.60 29.70 36.30
45.20 54.00 63.00 76.00
81.20
92.00
114.30
60.20
45.30 38.60 26.20 13.40
2.70
40.5 45.7 49.7 54.2
59.5 64.0 68.2 73.0
78.5 83.5
0.138 0.156 0.180 0.204
0.238 0.269 0.290 0.322
0.352 0.384 0.441 0.486
0.500 0.530 0.600 0.459
0.356 0.319
3.68
5.03
7.35
10.18
13.50 17.40 23.20 27.60
31.40 40.00
88.2
44.00
95.0
35.80
96.5 100.0
20.80 . 14.32
103.0 90.2
79,5 75.2 65.5
•
r
51.7
Spacing, 91.5 cm.
Radius, 0.914 cm.
Total cond. length, 0.0815 km.
S - 1.002.
244
DIELECTRIC PHENOMENA
Teat 33S
Teit 4 IS
Eff. kv. to neutral, «•
Amp. per km.
Loss kw./km., p
Eff. kv. to neutral, en
Amp. per km.
Loes kw./km., p
24.7
0.31 1.53 2.45 3.50
4.96 6.37 9.67 12.9
15.5 20.8 34.8 29.6
15.3
28.3
35.5 41.0 48.6
53.7 59.0 63.8 69.4
73.6 71.9 60.1 54.2
69.9 67.0 47.0
29.8
0.071 0.108 0.184
0.208 0.234 0.265 0.306
0.353 0.325 0.244 0.210
0.250 0.224 0.161
2.72
32.6
4.90
35.6
10.40
39.3
13.25
43.7
17.50
47.6
23.40
51.5
30.02
66.3
35.70
60.2
34.10
65.5
19.86
67.0
13.66
54.4
19.35
16.30 8.87
Spacing, 61cm.
Radius, 0.0914 cm.
Total cond. length, 0.0815 km.
8 - 1.006.
Spacing, 61 cm.
Radius, 0.105 cm.
Total cond. length, 0.0423 km.
6 « 1.001.
DATA APPENDIX
245
Teet 45B
Test 47B
Eff. kv. to neutral, e»
Amp. per km.
1
LOSB
kw./km., p
Eff. kv. to neutral, e*
Amp. per km.
LOM
kw./km., p
22.3
0.06 ; 0.12 0.34 1.41 ,
1 1
2.70
4.78
8.10
10.70
14.70 19.50 1 24.80 1 30.10
1 1
37.20 ! 43.40 56.20 59.00
80.50 84.50 i 52.20 32.70 ;
45.0 50.0 54.5 60.5
65.7 70.5 75.5 79.0
87.0 91.7 96.5 93.5
90.0 82.0 75.8 58.0
42.6 40.0
0.080
0.100
' 0.104
0.37
25.8
0.74
29.7
1.90
35.7
5.76
39.5
0.152 0.174 0.205 0.230
9.13
44.2
12.60
50.2
16.30
54.0
18.75
59.5
26.80
64.5
31.40
69.0
38.20
74.0
0.321
34.10
m
79.7
29.80
82.7
21.70
88.7
16.20
98.0
4.22
99.7
0.49
103.0
0.24
86.7
75.5
Spacing, 61 cm.
Radius, 0.164 cm.
Total cond. length, 0.0185 km.
5 » 0.996.
Spacing, 91.5 cm.
Radius, 0.256 cm.
Total cond. length, 0.0815 km.
5 » 0.996.
16
246
DIELECTRIC PHENOMENA
Spacing, 61 cm.
Radius, 0.256 cm.
Total cond. length, 0.0815 km.
a - 1.00.
TeBt48fi
Teat 49B
Eff. kv. to neutral, tn
Amp. per km.
Loss kw./km., p
Eff. kv. to neutral, e.
Amp. per km.
Loss kw./km., t>
44.1
0.61 1.11 3.87 5.90
10.60 17.16 20.70 26.70
33.30 27.10 29.40 23.90
18.30
16.55
8.10
4.10
40.5 44.5 43.0
46.8
50.6 55.6 58.8 53.8
49.6 45.7 43.2 39.3
1.16
47.2
3.13
61.7
2.27
54.5
5.70
60.8
12.30
67.2
19.25
71.5
75.5
16.05
81.7
9.70
76.6
5.27
78.5
2.82
74.0
1.23
69.5
•
68.0
58.2
52.7
Spacing, 30.5 cm.
Radius, 0.256 cm.
Total cond. length, 0.0815 km.
a " 0.996.
DATA APPENDIX
247
Test 51B
Te8t54B
Eff. ky. to neutral, en
Amp. per km.
Loee
kw./km., p
1
Eff. kv. to neutral, e*
Amp. per km.
Loea
kw./km., p
62.5
0.159 0.190 0.220 0.261
0.318
9.15 14.55 20.10 28.45
40.20 49.70 34.60
22.10
5.65
10.20
15.75
19.30
25.5 31.8 37.7 42.7
47.1 57.0 63.2
69.7 76.5 78.7 84.5
89.3
95.0
99.1
102.2
97.2 92.0 87.0 76.7
82.0 72.1
0.051
68.0
72.0
0.06
78.0
0.30
87.3
0.30
91.5
0.49
82.0
1.03
72.8
1.81
56.0
0.152 0.164 0.184
0.210 0.238 0.263
5.08
61.5
6.48
67.2
12.22
70.2
17.20
23.90 28.40 31.90
26.00
20.90
16.50
5.82
9.10
2.67
Spacing, 61 cm. Spftcing, 91.5 cm.
Radius, 0.333 cm. Radius, 0.464 cm.
Total cond. length, 0.0817 km. Total cond. length, 0.0825 km.
6 » 0.999. 6 " 0.982.
AU 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.
ToBt No. 146. Tiine A^
1 Test No. 18. Line A
L
Kv. bet. lines
Amp.
Kw.
Kw. line loss, p
Kv. bet. , lines
Amp.
Kw.
Kw. line loss, p
63.5
0.056
0.07
0.01
80.0
0.040
0.12
0.01
80.5
0.077
0.12
0.02
90.0
0.100
0.16
0.02
90.1
0.092
0.15
0.02
101.1
0.107
0.20
0.04
107.5
0.113
0.30
0.12
112.0
0.113
0.25
0.05
115.2
0.121
0.35
0.14
121.6
0.123
0.30
0.06
126.2
0.135
0.63
0.37
129.5
0.131
0.35
0.07
134.2
0.146
0.85
0.55
140.0
0.146
0.49
0.16
142.5
0.154
1.29
0.95
150.0
0.160
0.76
0.38
150.0
0.164
1.95
1.45
160.0
0.172
1.60
1.17
158.0
0.173
2.69
2.25
152.0
0.162
0.90
0.51
166.1
0.185
4.00
3.48
164.2
0.174
2.00
1.55
165.0
.0.183
3.51
3.02
172.0
0.187
3.40
2.90
173.7
0.196
5.00
4.45
183.2
0.205
5.60
5.02
163.4
0.184
2.70
2.23
188.2
0.210
6.92
6.30
170.4
0.193
4.20
3.67
196.4
0.223
9.02
8.42
181.0
0.198
6.06
5.42
202.2
0.237
11.06
10.36
203.0
0.251
12.84
12.04
206.0
0.242
12.90
12.09
199.2
0.243
11.50
10.73
187.2
0.211
6.95
6.34
193.4
0.227
9.10
8.49
196.4
0.225
9.60
8.90
176.4
0.197
4.74
4.17
•
Total conductor length, 10
(9,500 cm.
165.6
0.184
2.70
2.21
Spacing, 310 cm.
162.8
0.180
2.38
1.81
No. 3/0 7-strandhard-dra^
m copper-
154.4
0.169
1.28
0.85
weathered cable, diam. ]
L.18 cm.
166.0
0.176
2.94
2.45
Temperature, wet, 16 deg dry, 18.5.
. C.
184.4
0.198
6.49
5.87
Barometer, 75.5 cm.
172.0
0.193 0.177
3.85 2.03
3.31 1.57
Bright sun, wind.
160.0
Test No. 146. T.ine A
L
146.2
0.162
0.80
0.42
Total conductor length, 10 Spacing, 310 cm.
^,500 cm.
138.0
0.150
0.52
0.19
No. 3/0 7-strand cable, dia
. 1.18 cm.
127.6
0.137
0.40
0.12
Temperature, wet, 24 deg.
C.
122.5
0.129
0.33
0.08
dry, 30 deg.
C.
111.2
0.117
0.25
0.04
Barometer, 75.7 cm.
101.0
0.105
0.20
0.03
Hazy.
^Thia 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
201.0 211.0 189.0 181.8
170.8 160.0 149.0 201.0
149.0 140.5 135.5 124.5
113.5 102.3
0.232
6.05
0.277
9.10
0.210
3.54
0.200
2.36
0.189
1.10
0.176
0.60
0.162
0.36
0.231
6.15
0.162
0.39
0.150
0.29
0.145
0.25
0.131
0.20
0.118
0.16
0.103
0.13
6.65 8.63 3.19 2.04
0.80 0.36 0.16 5.75
0.19 0.12 0.10 0.08
0.08 0.07
Total conductor length, 109,500 cm. Spacing, 310 cm.
No. 3/0 7H3trand 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
Kv. bet. lines
Amp.
Kw.
Kw. line loas, p
Test No. 105, Line A
Kv. bet. lines
Amp.
Kw.
Kw. line loss, p
120.0
129.0 160.0 181.0
189.0 203.0 213.0 205.0
0.138 0.150 0.175 0.202
0.212 0.237 0.252 0.239
0.24 0.30 0.78 3.65
4.65
7.84
11.20
8.70
0.15 0.19 0.61 3.40
4.36
7.48
10.78
8.18
Total conductor length, 108,500cm. Spacing, 310 cm.
No. 3/0 7Hstrand cable (H. D. copper- weathered), 1.18 cm. Temperature, wet, 1 deg. C.
dry, 3 deg. C. Barometer, 75.2 cm. Cloudy.
79.8
90.7
101.5
109.5
120.5 130.0 141.5 147.0
153.6 159.0 169.8 174.0
181.0 186.2 192.6 200.6
208.6 216.0 221.0 227.0
234.0 189.0 195.0 203.8
212.0 219.0
0.080 0.093 0.106 0.114
0.127 0.139 0.154 0.165
0.168 0.178 0.199 0.190
0.198 0.204 0.212 0.221
0.237 0.247 0.259 0.271
0.288 0.210 0.217 0.229
0.242 0.257
0.03 0.04 0.06 0.08
0.10 0.14 0.19 0.21
0.25 0.30 0.51 0.70
1.20 1.74 2.70 4.00
5.60
7.40
9.00
11.00
13.60 2.30 3.10 4.96
6.70 8.60
0.01 0.01 0.02 0.03
0.04 0.06 0.09 0.08
0.12 0.16 0.35 0.53
1.02 1.55 2.49 3.77
5.34
7.13
8.70
10.66
13.25 2.10 2.88 4.72
6.44 8.31
Total conductor length, 109,500 cm. Spacing, 310 cm.
No. 3/0 7-8trand 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. T.ine B
Test No.
73, Line B
Kv. bet. lines
Amp.
Kw.
Kw. line loss, p
Kv. bet. lines
Amp.
Kw.
Kw. line lose, p
67.0
0.025 0.028
0.02 0.03 0.05
0.02 0.02 0.02
43.0 60.0 69.7
0.016 0.022 0.026
77
88.0
0.08
0.06
98.9
0.035
0.07
0.03
80.6
0.030
.0.10
0.07
109.5
0.040
0.12
0.07
90.5
0.034
0.15
0.11
119.5
0.043
0.22
0.14
101.5
0.038
0.30
0.26
128.0
0.050
0.42
0.32
91.0
0.034
0.09
0.05
137.0
0.054
0.90
0.78
90.5
0.034
0.10
0.06
144.0
0.060
1.94
1.80
70.3
0.026
0.06
0.04
161.2
0.078
4.50
4.31
101.6
0.038
0.17
0.12
153.0
0.070
3.04
2.88
101.6
0.038
0.17
0.12
173.8
0.090
6.60
6.47
109.5
0.041
0.40
0.36
185.0
0.103
8.72
8.36
105.5
0.040
0.14
0.09
200.0
0.106
11.90
11.59
115.0
0.040
0.14
0.09
185.0
0.103
8.76
8.50
115.0
0.0425
0.88
0.82
159.0
0.078
4.10
3.92
121.5
0.048
0.16
0.09
139.0
0.058
1.22
1.10
126.5
0.053
2.00
1.93
161.2
0.080
4.70
4.51
130.5
0.055
2.48
2.40
211.8
0.135
14.80
14.46
140.5
0.064
3.70
3.61
144.5
073
4.26
4.16
Total condui Spacing, 91. 0.375-in. g
Btor leng 4 cm. Eilv. ste<
th, 29,05 3l cable,
cm. diam.
^ ^ ^ ■ %^
70.5
91.5
106.0
^0 • %# • 1^
0.030 0.038
0.03 0.06 0.18
0.00 0.02 0.13
0.953 cm. Temperatur
Barometer, ' Cloudy.
e wet, 1
dry, 1
74.7 cm.
deg. C. deg. C.
150.0
156.4 161.0 166.0
0.078
0.083 0.089 0.093
4.80
5.80 6.72 7.50
4.69
. 5.68 6.67 7.36
Total con Spacing, 0.23-in. 1
iductor 1 91.4 cm. galv. at
ength, 2< eel cab]
9,050 cm. e, diam.
0.585 c
m.
Temperal Baromete
iure wetj
dry,
r, 75.2 c
, 1 deg. { 3deg. (
Cloudy.
252
DIELECTRIC PHENOMENA
Test No. 79, Line B
Kv. bet. linee
Amp.
Kw.
Kw. line loefl, p
Test No. 80. Line B
Kv. bet. linee
Amp.
Kw.
Kw. line loM, p
213.0 205.0 202.0 186.0
181.0 168.4 159.6 150.0
138.0 120.0 120.0 110.0
99.0
0.105
8.64
0.010
7.68
0.094
7.40
0.088
6.00
0.081 0.072 0.063 0.058
0.048 0.043
5.00 3.96 3.00 2.24
1.14 0.20 0.26 0.19
0.13
8.38 7.40 7.13 5.80
4.80 3.81 2.88 2.13
1.06 0.14 0.20 0.14
0.09
Total conductor length, 29,050 cm.
Spacing, 244 cm.
0.23-in. galv. steel cable, diam. 0.585
cm. Temperature, wet, 1 deg. C.
dry, 3 deg. C. Barometer, 72.5 cm. Cloudy.
81.0
0.029
0.07
91.0
0.032
0.09
100.5
0.035
0.12
110.5
0.038
0.16
120.5
0.041
0.40
130.5
0.048
1.30
139.5
0.055
2.25
153.0
0.067
3.20
160.0
0.075
4.40
172.0
0.084
6.70
181.0
0.094
7.00
192.0
0.103
8.50
199.0
0.109
9.40
213.0
1
0.124
11.70
0.04 0.05 0.07 0.11
0.34 1.22 2.17 3.09
4.28 5.54 6.82 8.28
9.15 11.38
Total conductor length, 29,050 cm.
Spacing, 152 cm.
0.23-in. galv. steel cable, diam.
0.585 cm. Temperature, wet, 1 d^. C.
dry, 3 deg. C. Barometer, 72.5 cm. Cloudy.
DATA APPENDIX
253
Corona Loss — Outdoor Line — 60-ctclb
Test No. 125. Line B
Test No. 126. Line B
Kv. bet. lines
Amp.
Kw.
Kw. line loee,p
Kv. bet. lines
Amp.
Kw.
Kw. line loes, p
80.0
0.025
0.06
0.05
100.0
0.031
0.12
0.09
88.0
0.031
0.13
0.11
110.0
0.037
0.22
0.17
101.0
0.037
0.32
0.29
119.0
0.041
0.44
0.36
110.0
0.041
0.74
0.68
131.0
0.050
1.36
1.22
120.0
0.050
1.67
1.59
142.0
0.056
2.38
2.16
128.0
0.056
2.56
2.44
151.0
0.065
3.23
2.92
140.0
0.067
4.00
3.80
160.0
0.074
4.20
3.78
150.0
0.08
5.42
5.12
171.0
0.082
5.45
4.93
159.6
0.09
6.86
6.46
181.0
0.09
6.56
5.89
168.4
0.101
8.30
7.80
194.0
0.102
8.20
7.34
181.0
0.112
10.36
9.68
202.0
0.111
9.26
8.30
190.0
0.122
12.24
11.44
212.0
0.117
10.84
9.74
201.0
0.134
14.68
13.61
222.0
0.128
12.44
11.18
213.0
0.14a
17.28
16.14
231.0
0.135
13.80
12.38
206.0
0.144
15.76
14.72
225.0
0.129
12.88
11.58
196.6
0.128
13.60
12.70
217.0
0.124
11.64
10.45
186.2
0.117
11.44
10.69
205.0
0.112
9.70
8.70
175.0
0.103
9.20
8.59
196.6
0.104
8.56
7.68
165.6
0.096
7.76
7.27
186.6
0.096
7.32
6.56
153.4
0.083
5.92
5.57
176.0
0.086
6.12
5.51
143.0
0.074
4.56
4.33
165.0
0.078
4.96
4.49
134.0
0.064
3.34
3.18
156.4
0.069
3.96
3.59
123.0
0.053
2.00
1.90
142.4
0.056
2.46
2.24
114.0
0.044
1.00
0.94
134.0
0.051
1.60
1.45
104.0
0.038
0.38
0.34
125.0
0.044
0.82
0.71
Total condu
ctor leng
th, 29,06
cm.
Total conductor length, 2
!9,050 cm.
Spacing, 91.
4 cm.
Spacing, 183 cm.
No. 4 H. D
. copper
wire, dii
am. 0.518
No. 4 H. D. copper wi
ire, diam.
cm.
0.518 cm.
Tc^mperatuT
e, wet, i
5.0 deg. <
C.
Temperature, wet, 5.0 dq
- C.
dry, ^
L6 deg. <
c.
dry, 4.5 dej
- C.
Barometer,
75.9 cm.
Barometer, 75.9 cm.
Cloudy, 8lig
ht breez<
B.
Cloudy, slight breeze.
254
DIELECTRIC PHENOMENA
Test No. 137, Line B
Kv. bet. lines
Amp.
Kw.
Kw. line
lOM, p
Teet No. 138, Line B
Kv. bet. lines
Amp.
Kw.
Kw. line loM. V
80.0
go. 5
100.5 110.7
121.0 131.0 141.5 150.8
161.0 172.0 183.0 196.0
205.0 202.0 186.0 165.0
145.0 124.0 103.0
0.05
0.025
0.11
0.020
0.35
0.037
0.95
0.044
1.42
0.051
2.11
0.056
2.70
0.064
3.24
0.072
4.05
0.078
4.80
0.084
5.60
0.093
6.60
0.102
7.60
0.098
7.30
0.087
6.00
0.075
4.30
0.061
2.86
0.047
1.75
0.032
0.60
0.02 0.06 0.26 0.78
1.19 1.76 2.26 2.72
3.40 4.05 4.73 5.59
6.44 6.19 5.08 3.63
2.40 1.46 0.47
Total conductor lengthi 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. Barometer, 76.6 cm. Bright sun, slight breeze.
79.2
91.2
99.9
111.4
120.8 121.5 141.0 149.0
161.0 171.4 181.4 192.0
202.2 214.4 197.0 174.0
153.2 134.4
0.025 0.027 0.036
0.039 0.049 0.055 0.059
0.066 0.074 0.079 0.085
0.092 0.11 0.089 0.076
0.063 0.051
0.06 0.12 0.26 0.08
1.22 1.90 2.30 2.80
3.40 4.20 4.80 5.60
6.56 7.50 6.10 4.40
3.00 2.00
0.03 0.07 0.18 0.65
1.06 1.59 2.20 2.34
2.85 3.53 4.05 4.73
5.67 6.36 5.15 3.71
2.51 1.67
Total conductor length, 29,050 cm.
Spacing, 488 cm.
No. 8 new H. D. copper wire, diam.
0.328 cm. Temperature, wet, — 1.5 deg. C.
dry, + 1.5 deg. C, Barometer, 75.5 cm. Bright sun, slight breeze.
DATA APPENDIX
255
Test No. 92. Line B
Kv. bet. lines
51.0 56.5 61.6 66.5
71.0 76.0 83.0 90.5
101.0 110.5 120.5 131.5
144.5 158.0 170.0 181.0
190.0 204.0 215.0 222.0
Amp.
27.5
0.008
34.5
0.009
39.5
0.011
44.5
0.013
0.015 0.017 0.019 0.023
0.024 0.028 0.032 0.037
0.041 0.050 0.055 0.060
0.068 0.081 0.086 0.094
0.099 0.110 0.117 0.123
Kw.
0.02
0.05 0.10 0.22 0.37
0.49 0.60 0.81 1.07
1.43 1.80 2.30 2.80
3.50 4.40 5.30 6.18
6.70 8.00 9.00 9.64
Kw. line loas, V
0.01
0.04 0.09 0.20 0.31
0.40 0.49 0.66
0.88
1.17 1.46 1.88 2.28
2.84 3.57 4.33 5.15
5.43 6.50 7.30
7.84
Total conductor length, 29,050 cm.
Spacing, 410 cm.
0.066-in. galv. steel wire, diam. 168
cm. Temperature, wet, 0.5 deg. C.
dry, 2.0 deg. C. Barometer, 75.0 Cloudy, no wind.
Teat No. 95. Line B
Kv. bet. linee
Amp.
KV7.
Kw. line loaa, p
222.0 199.8 181.0 158.0
140.0
120.0
102.0
91.5
79.5 68.7 60.0 50.0
0.115
8.80
0.104
6.80
0.089
5.36
0.076
3.80
0.064
2.84
0.053
1.92
1.21
0.034
0.93
0.028
0.63
0.021
0.63
0.017
0.18
0.014
7.00 5.38 4.24 2.98
2.24 1.44 0.96 0.75
0.51 0.52 0.16
Total conductor length, 29,050 cm.
Spacing, 550 cm.
0.066 in. galv. steel wire, diam.
168 cm. Temperature, wet, 1.0 deg. C.
dry, 3.0 deg. C. Barometer, 75.0 cm. Cloudy, no wind.
256
DIELECTRIC PHENOMENA
Transformer Loss
Kv.
AmperoB
Kw.
Kv.
Amperes
Kw.
101.5
0.008
71.5
0.005
0.02
131.5
0.010
0.15
82.0
0.006
0.03
147.3
0.011
0.25
97.0
0.007
0.05
112.0
0.008
0.06
163.8
0.013
0.42
132.8
0.009
0.09
181.5
0.014
0.54
201.8
0.016
0.69
149.0
0.010
0.12
178.4
0.013
0.18
30*»C.
201.0
0.014
0.22
223.0
0.016 3'»C.
0.30
INDEX
A
Pagk
Air, at very low pressures 196
compressed 42
density 51
occluded in solid insulation 236
see Ck>rona. Altitude, effect of, on arc-over of bushings, leads and insulators. . Ill, 217
effect of I on corona 42, 50, 51
effect of, on corona loss 146
effect of, on sphere-gap spark-over ' . 96
variation of air density with 51
B
Barriers in oil 169, 189
Beta particle 193
Bushing, condenser type 220
effect of altitude on spark-over of Ill
oil-filled type 220
overstressed air in 217
rod and torus 220
transformer 220
C
Cable, graded 33, 218
Capacity, see 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 spark or 27, 79, 84
in oil 155
Corona loss, a.c. and d.c 132
description of experimental lines 117
disruptive critical voltage 137
effect of frequency 129
effect of humidity, initial ionization, etc 147, 148
effect of moisture, frost, fog, sleet, rain and snow 145, 149
257
258 INDEX
Paob
Corona loss, effect of smoke and wind 149
effect of temperature and barometric pressure 146
for small conductors 136, 137, 140, 142
law of 134, 137, 140, 142
loss near the disruptive critical voltage 143
\ probability law 148, 162
quadratic law 121
Clorona, on generator coils 216
Corona on transmission lines, see Transmission lines.
Corona, visual, a.c. and d.c 38, 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, 58, 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
influence of frequency on 65
on conductors close together 77
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
stroboscopic study of 73
Cylinders, concentric, flux density 13
gradient 13, 29
permittance or capacity 13, 29
visual corona, see Visual corona 38 el seg.
spark-over and corona in oil 159
parallel, see Wires.
INDEX 269
D
Page
Dielectrici addition of fluxes 14
circuit 216
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
formula for different electrodes 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 26
equation of lines of force between parallel wires 20
equation of lines of force from spheres 26
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 163
soUd 166
E
Elastance 11, 215
Elastivity 11, 216
260 INDEX
Page
Electron theory , application of, to visual corona 41y^7, 194
general discussion of 192
practical application of 194
Energy distance 41, 42, 48, 67, 156, 195
Equipotential surfaces, construction of 226
equation of, for parallel wires 16
equation of, for spheres 25
in three dimensions 232
Experimental study of, corona loss 117
dielectric fields 2, 232
solid insulations 166
spark-over. 79
strength of oil 163
visual corona 44
Flux, see Dielectric flux.
Frequency, effect on corona loss 129, 162
effect on visual corona 66
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 pomt 230
at different points around a conductor 231
Provenance
- Shelf
- Reference library
- Author
- F.W. Peek Jr.
- Rights
- Published in 1915, before 1929, and therefore in the public domain in the United States.
- Collected By
- StanBot reference library