where

L = inductance of a loop of a three phase circuit in henrys.

Note.—The inductance of a complete single phase circuit = L × 2 ÷ √3.

A = distance between wires;
d = diameter of wire.

Size B.&S. Diam.
(inches)
Distance
d
(inches)
Capacity
C
(μfarads)
0000 .46 12.0226
18.0204
24.01922
48.01474
000 .41 12.0218
18.01992
24.01876
48.01638
00 .365 12.0124
18.01946
24.01832
48.01604
0 .325 12.02078
18.01898
24.01642
48.01570
1 .289 12.02022
18.01952
24.01748
48.0154
2 .258 12.01972
18.01818
24.01710
48.01510
3 .229 12.01938
18.01766
24.01672
48.01480
4 .204 12.01874
18.01726
24.01636
48.01452
5 .182 12.01830
18.01690
24.01602
48.01426
6 .162 12.01788
18.01654
24.01560
48.0140
7 .144 12.01746
18.01618
24.01538
48.01374
8 .128 12.01708
18.01586
24.01508
48.01350
9 .114 12.01660
18.01552
24.01478
48.01326
10 .102 12.01636
18.01522
24.01452
48.01304

Capacity.—In any given system of electrical conductors, a pressure difference between two of them corresponds to the presence of a quantity of electricity on each. With the same charges, the difference of pressure may be varied by varying the geometrical arrangement and magnitudes and also by introducing various dielectrics. The constant connecting the charge and the resulting pressure is called the capacity of the system.

All circuits have a certain capacity, because each conductor acts like the plate of a condenser, and the insulating medium, acts as the dielectric. The capacity depends upon the insulation.

For a given grade of insulation, the capacity is proportional to the surface of the conductors, and universally to the distance between them.

A three phase three wire transmission line spaced at the corners of an equilateral triangle as regards capacity acts precisely as though the neutral line were situated at the center of the triangle.