232 HANDBOOK OF ELECTRICAL ENGINEERING
Table 9.28. Cable data for the worked example
Cable conductor
area (mm^2 )
Resistance at 90◦C
(ohm/km)
Reactance at 60 Hz
(ohm/km)
0. 033 r+ 0. 944 x
(ohm/km)
95 0.247 0.0872 0.16383
120 0.197 0.0868 0.14694
150 0.160 0.0874 0.13531
185 0.128 0.0876 0.12493
240 0.0989 0.0866 0.11439
300 0.0802 0.0860 0.10765
Hence from Tables 9.16 and 9.17 the small size of cable could be 95 mm^2. Table 9.28 can be prepared
for cables of 95 mm^2 and above, routed in air.
Hence a 300 mm^2 would be necessary for the starting duty. Check the actual volt-drop for
both starting and running currents.
Vstart=
√
31408 ( 0. 0802 × 0. 33 + 0. 086 × 0. 944 ) 0. 25 × 100
440
= 14. 92 = 14 .9%
Vrun=
√
3245. 4 ( 0. 0802 × 0. 92 + 0. 086 × 0. 3919 ) 0. 25 × 100
440
= 2. 596 = 2 .6%
The choice of a 300 mm^2 may just be acceptable for a running volt-drop of 2.6%, but satisfies
the required starting volt-drop.
Calculate the cut-off capability of the 400 A fuses. The same approach is used as in the
previous Example 9.4.3.5.1. The fault impedanceZfin (9.8) is higher due to operation of only one
transformer,
Zf=Zbs+Zt= 0. 001054 +j 0 .006821 ohms/phase
The magnitude of this is 0.006902 ohms/phase, which has anX/Rratio of 6.4715. The dou-
bling factor is,
D=
√
2
[
1. 0 +e
−π
6. 4715
]
= 2. 2846
The prospective RMS fault current at or near to the fuses isIf,
If=
Vos
√
3 Zf
=
460
√
3 × 0. 006902
=38478.9 amps
Hence the peak value of the symmetrical fault current
Ifpka= 2. 2846 × 38478. 9 =87908.8 amps