In the given circuit of figure, with steady current, the potential drop across the capacitor must be
A
V
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B
V/2
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C
V/3
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D
2V/3
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Solution
The correct option is BV/3 When the capacitor is fully charged, no current draws from cell. So, the current will flow in the outer loop. Now applying KVL for this loop we get, 2V−V=(2R+R)I or I=(V/3R) Thus, VDE=2V−2RI=2V−2R(V/3R)=(4V/3) Potential across C is VAB=VDE−V=4V/3−V=V/3