Solution: Let us find current in branch CD, that is,
I due to the voltage source in branch AB as in
Figure 5.99.
Applying KVL in mesh I, we get the following:
3 (i
1
−i
2
) = 10
or
ii
12
–=
10
3
i
1
−i
2
= 3.33 (5.26)
Applying KVL in mesh II, the following form can
be obtained:
3(i
2
−i
1
) + (−j10) (i
2
−i
3
) = 0
or − 3i
1
+ (3 −j10) i
2
+j10 i
3
= 0 (5.27)
Applying KVL in mesh III, the equation can be written as follows:
−J10 (i
3
−i
2
) + (2 +j5) i
3
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