VAB–Ais calculated by integrating the electric field intensity, due to the charge on conductor A, on
conductor B fromrAtoD
VABA¼
ðD
rA
EAdx¼
q
2 p« 0
ln
D
rA
(13:65)
VAB–Bis calculated by integrating the electric field intensity due to the charge on conductor B fromDtorB
VABB¼
ðrB
D
EBdx¼
q
2 p« 0
ln
rB
D
hi
(13:66)
The total voltage is the sum of the generated voltagesVABAandVABB
VAB¼VABAþVABB¼
q
2 p« 0
ln
D
rA
q
2 p« 0
ln
rB
D
hi
¼
q
2 p« 0
ln
D^2
rArB
(13:67)
If the conductors have the same radius,rA¼rB¼r, then the voltage between conductorsVAB, and the
capacitance between conductorsCAB, for a 1-m line length are
VAB¼
q
p« 0
ln
D
r
ðÞV (13:68)
CAB¼
p« 0
ln
D
r
ðÞF=m (13:69)
The voltage between each conductor and ground (G) (Fig. 13.16) is one-half of the voltage between the two
conductors. Therefore, the capacitance from either line to ground is twice the capacitance between lines
VAG¼VBG¼
VAB
2
ðÞV (13:70)
CAG¼
q
VAG
¼
2 p« 0
ln
D
r
ðÞF=m (13:71)
CAG
A
CBG
VAG VBG
VAB
+
q−
q−
q+
q+
−
B
VBG
VAG
VAB
CAG
CBG
B
A
−
FIGURE 13.16 Capacitance between line to ground in a two-wire single-phase line.