In the circuit of Fig. 1, use Millman’s theorem to find current through the 4 Ω resistance.
The given circuit can be redrawn as shown in Fig. 2. In the circuit of Fig. 2 each voltage source has a series resistance which can be considered as internal resistance of the source. Hence, the parallel connected voltage sources with internal resistance can be converted into a single equivalent source using Millman’s theorem.
Let Eeq=Equivalent emf of parallel connected sources
Req=Equivalent internal resistance.
Now, by Millman’s theorem,
Req=R11+R21+R311=81+21+10111=0.7251=1.3793Ω
Eeq =(R1E1+R2E2+R3E3)Req
=(820+210+105)×1.3793=11.0344V
The circuit of Fig. 2 can be redrawn as shown in Fig. 3. Let, I be the current through 4 Ω resistance. With reference to Fig. 3, by Ohm’s law we can write,
I=Req+4Eeq=1.3793+411.0344=2.0513A
RESULT
Current through 4 Ω resistance = 2.0513 A