Q142 / 150 · MHT CET 2026 (19 April Shift 1) · Physics
A slab of material of dielectric constant $K$ has the same area as the plates of a parallel plate capacitor but has a thickness $(4/5)d$, where $d$ is the separation of the plates. The capacitance in the presence and absence of dielectric are $C$ and $C_0$ respectively. The ratio $(C/C_0)$ is
- A$\dfrac{K + 4}{5K}$
- B$\dfrac{4K}{K + 5}$
- Correct answerC$\dfrac{5K}{K + 4}$
- D$\dfrac{K + 5}{4K}$
Solution
The capacitance of a parallel plate capacitor without a dielectric is given by:
$C_0 = \dfrac{\varepsilon_0 A}{d}$
When a dielectric slab of thickness $t$ and dielectric constant $K$ is introduced, the capacitance becomes:
$C = \dfrac{\varepsilon_0 A}{d - t + \dfrac{t}{K}}$
Given $t = \dfrac{4}{5}d$, substituting this value yields:
$C = \dfrac{\varepsilon_0 A}{d - \dfrac{4}{5}d + \dfrac{4d}{5K}}$
$C = \dfrac{\varepsilon_0 A}{\dfrac{d}{5} + \dfrac{4d}{5K}}$
$C = \dfrac{\varepsilon_0 A}{\dfrac{d(K + 4)}{5K}}$
$C = \dfrac{5K \varepsilon_0 A}{d(K + 4)}$
Taking the ratio of $C$ to $C_0$ gives:
$\dfrac{C}{C_0} = \dfrac{5K}{K + 4}$
Answer: $\dfrac{5K}{K + 4}$
$C_0 = \dfrac{\varepsilon_0 A}{d}$
When a dielectric slab of thickness $t$ and dielectric constant $K$ is introduced, the capacitance becomes:
$C = \dfrac{\varepsilon_0 A}{d - t + \dfrac{t}{K}}$
Given $t = \dfrac{4}{5}d$, substituting this value yields:
$C = \dfrac{\varepsilon_0 A}{d - \dfrac{4}{5}d + \dfrac{4d}{5K}}$
$C = \dfrac{\varepsilon_0 A}{\dfrac{d}{5} + \dfrac{4d}{5K}}$
$C = \dfrac{\varepsilon_0 A}{\dfrac{d(K + 4)}{5K}}$
$C = \dfrac{5K \varepsilon_0 A}{d(K + 4)}$
Taking the ratio of $C$ to $C_0$ gives:
$\dfrac{C}{C_0} = \dfrac{5K}{K + 4}$
Answer: $\dfrac{5K}{K + 4}$
Hence, the correct answer is option: 'C'.