Capacitors

JEE Main level, single correct, medium

114 of 180

Question 114 of 180

The space between the plates of a parallel plate capacitor is filled with a 'dielectric' whose 'dielectric constant' varies with distance as per the relation:
K(x)=Ko+λx(λ=a constant )\mathrm{K}(\mathrm{x})=\mathrm{K}_{\mathrm{o}}+\lambda \mathrm{x}(\lambda=\mathrm{a} \text { constant })
The capacitance
C\mathrm{C}, of the capacitor, would be related to its vacuum capacitance Co\mathrm{C}_{\mathrm{o}} for the relation :

Show answer and solution

Answer: (C) C=λdln⁡(1+λd/KoCo)\left.\mathrm{C}=\frac{\lambda \mathrm{d}}{\ln \left(1+\lambda \mathrm{d} / \mathrm{K}_{\mathrm{o}}\right.} \mathrm{C}_{\mathrm{o}}\right)

The value of dielectric constant is given as,
K=K0+λx And, V=∫0dEdrV=∫0dσKdx\begin{aligned} &\mathrm{K}=\mathrm{K}_0+\lambda \mathrm{x} \\ &\text { And, } \mathrm{V}=\int_0^{\mathrm{d}} \mathrm{Edr} \\ &\mathrm{V}=\int_0^{\mathrm{d}} \frac{\sigma}{\mathrm{K}} \mathrm{dx} \end{aligned}

=σ∫0d1( K0+λxdx=σλ[ln⁡(K0+λd−ln⁡K0]=σλln⁡(1+λdK0)\begin{aligned} &=\sigma \int_0^{\mathrm{d}} \frac{1}{\left(\mathrm{~K}_0+\lambda \mathrm{x}\right.} \mathrm{dx} \\ &=\frac{\sigma}{\lambda}\left[\ln \left(\mathrm{K}_0+\lambda \mathrm{d}-\ln \mathrm{K}_0\right]\right. \\ &=\frac{\sigma}{\lambda} \ln \left(1+\frac{\lambda \mathrm{d}}{\mathrm{K}_0}\right) \end{aligned}
Now it is given that capacitance of vacuum
=C0=\mathrm{C}_0.
Thus,
C=QV\mathrm{C}=\frac{\mathrm{Q}}{\mathrm{V}}
=σ.sv( Let surface area of plates =s)=σ.sσλln⁡(1+λdK0)\begin{aligned} &=\frac{\sigma . \mathrm{s}}{\mathrm{v}}(\text { Let surface area of plates }=\mathrm{s}) \\ &=\frac{\sigma . \mathrm{s}}{\frac{\sigma}{\lambda} \ln \left(1+\frac{\lambda \mathrm{d}}{\mathrm{K}_0}\right)} \end{aligned}
=sλ⋅dd1ln⁡(1+λdK0)(∵=\mathrm{s} \lambda \cdot \frac{\mathrm{d}}{\mathrm{d}} \frac{1}{\ln \left(1+\frac{\lambda \mathrm{d}}{\mathrm{K}_0}\right)}\left(\because\right. in vacuum ε0=1)\left.\varepsilon_0=1\right)
c=λdln⁡(1+λdK0)⋅C0(\mathrm{c}=\frac{\lambda \mathrm{d}}{\ln \left(1+\frac{\lambda \mathrm{d}}{\mathrm{K}_0}\right)} \cdot \mathrm{C}_0 \quad\left(\right. here, C0=sd)\left.\mathrm{C}_0=\frac{\mathrm{s}}{\mathrm{d}}\right)

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