A slab of material of dielectric constant k, having the same area as the plate of a parallel plate capacitor but has a thickness $\frac{3}{5}$ of the distance between the plates d, is inserted between the plates of the capacitor. When there is air between the plates, the potential difference is $V_0$. What is the potential difference between the plates of the capacitor after inserting the dielectric? |
$\left(\frac{2 k+3}{k}\right) V_0$ $\left(\frac{2 k+3}{5 k}\right) V_0$ $\left(\frac{5 k}{2 k+3}\right) V_0$ $\left(\frac{k+3}{5 k}\right) V_0$ |
$\left(\frac{2 k+3}{5 k}\right) V_0$ |
The correct answer is Option (2) → $\left(\frac{2 k+3}{5 k}\right) V_0$ Capacitance without Di-electric, $C_0=\frac{ε_0}{d}$ Now, $C_1$ (Capacitance with Dielectric) = $\frac{Kε_0A}{d/3}=3.\frac{Kε_0A}{d}$ $C_2$ (Capacitance without Dielectric) = $\frac{Kε_0A}{2d/3}=\frac{3ε_0A}{2d}$ $∴\frac{1}{C}=\frac{1}{C_1}+\frac{1}{C_2}$ [Connected in series] $\frac{1}{C}=\frac{d}{3Kε_0A}+\frac{2d}{3ε_0A}$ $⇒C=\frac{3ε_0A}{d\left(\frac{1}{k}+2\right)}$ Also, $V=\frac{Q}{C}=\frac{C_0V_0}{C}=\frac{\frac{ε_0}{d}V_0}{\frac{3ε_0A}{d\left(\frac{1}{k}+2\right)}}$ $=\frac{V_0}{3\left(\frac{1}{k}+2\right)}$ |