An ideal cell of emf $10 \mathrm{~V}$ is connected in circuit shown in figure. Each resistance is $2 \Omega$. The potential difference (in V) across the capacitor when it is fully charged is
- $\mathrm{R}_{1}$ to $\mathrm{R}_{5} \rightarrow$ each $2 \Omega$
- Cap. is fully charged
- So no current is there in branch ADB
- Effective circuit of current flow :
$\mathrm{R}_{e q}=\left(\frac{4 \times 2}{4+2}\right)+2$
$\mathrm{R}_{e q}=\frac{4}{3}+2=\frac{10}{3} \Omega$
$\mathrm{i}=\frac{10}{10 / 3}=3 \mathrm{~A}$
So potential different across $\mathrm{AEB}$
$\Rightarrow 2 \times 1+2 \times 3=8 \mathrm{~V}$
Hence potential difference across
Capacitor $=\Delta \mathrm{V}=\mathrm{V}_{\mathrm{AEB}}=8 \mathrm{~V}$
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