The network shown in the figure above consists of four identical batteries and 11 unknown resistors. When an ideal ammeter is connected between the terminals A and B, its reading is 2 A and when a resistance of is connected in series with the ammeter its reading becomes . Now the ammeter and the resistance are disconnected and an ideal voltmeter is connected between the terminals A and B. What would the voltmeter read?
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By Thévenin's theorem , any circuit of voltage sources and resistors with two terminals can be transformed into an equivalent circuit of a voltage source and a resistance (see left figure above). From the equivalent circuits above, we have:
⎩ ⎪ ⎨ ⎪ ⎧ R T h V T h = 2 R T h + 2 V T h = 1 ⟹ V T h = 2 R T h ⟹ V T h = R T h + 2 . . . ( 1 ) . . . ( 2 )
( 1 ) = ( 2 ) : 2 R T h ⟹ R T h ( 1 ) : V T h = R T h + 2 = 2 Ω = 2 R T h = 4 V