
In steady state, a capacitor of capacitance $2 \mu \mathrm{F}$ is charged to $4 \mu \mathrm{C}$, as shown in…

- $4 \mathrm{~V}$
- $5 \mathrm{~V}$
- $2.5 \mathrm{~V}$
- $2 \mathrm{~V}$
Solution

$ \mathrm{V}_C=\frac{Q}{C}=\frac{4 \times 10^{-6}}{2 \times 10^{-6}}=2 \mathrm{v} $ Now, $\mathrm{V}_C=\mathrm{V}$ (across $2 \Omega$ resistor) $ \therefore \quad I=\frac{V}{R}=\frac{2}{2}=1 \mathrm{~A} $ Now, using the relation, $\mathrm{V}=E-I r$ So, $\mathrm{E}=V+I r=2+1 \times 0.5=2.5 \mathrm{~V}$
Asked in: AP EAMCET 2017 (26 Apr Shift 1)