A parallel plate capacitor has the space between its plates filled by two slabs of thickness \((\mathrm{d} / 2)\) each and dielectric constant \(\mathrm{K}_{1}\) and \(\mathrm{K}_{2}\) If \(\mathrm{d}\) is the plate separation of the capacitor, then capacity of the capacitor is .......... (A) $\left[\left(2 \mathrm{~d} \in_{0}\right) / \mathrm{A}\right]\left[\left(\mathrm{K}_{1}+\mathrm{K}_{2}\right) /\left(\mathrm{K}_{1} \mathrm{~K}_{2}\right)\right]$ (B) $\left[\left(2 \mathrm{~A} \in_{0}\right) / \mathrm{d}\right]\left[\left(\mathrm{K}_{1} \mathrm{~K}_{2}\right) /\left(\mathrm{K}_{1}+\mathrm{K}_{2}\right)\right]$ (C) $\left[\left(2 \mathrm{Ad} \epsilon_{0}\right) / \mathrm{d}\right]\left[\left(\mathrm{K}_{1}+\mathrm{K}_{2}\right) /\left(\mathrm{K}_{1} \mathrm{~K}_{2}\right)\right]$ d] \(\left(K_{1}+K_{2}\right)\) (D) \(\left[\left(2 \mathrm{~A} \in_{0}\right) /\right.\)

Short Answer

Expert verified
The capacity of the capacitor is given by (B) \(\left[\left(2 \mathrm{~A} \epsilon_{0}\right) / \mathrm{d}\right]\left[\left(\mathrm{K}_{1} \mathrm{~K}_{2}\right) /\left(\mathrm{K}_{1}+\mathrm{K}_{2}\right)\right]\).

Step by step solution

01

Understanding the problem

The key to this problem is understanding that the two dielectric slabs share the capacitor space evenly. Given that each slab has a thickness of \(d / 2\), they totally cover up the space between the capacitor plates. Since the slabs have different dielectric constants, we need to compute the capacitance contribution of each slab separately, and then compute the overall capacitance.
02

Finding the capacitance of each slab

The capacitance for each capacitor slab can be computed using the formula for capacitance of a parallel plate capacitor, which is \(C = \frac{\kappa \epsilon_0 A}{d}\). Since the dielectric fills half the distance between the plates for each slab, the thickness \(d/2\) should be used in the formula. Therefore, the capacitance for the dielectrics with dielectric constants \(K_1\) and \(K_2\) would be \(C_1 = \frac{K_1 \epsilon_0 A}{d/2}\) and \(C_2 = \frac{K_2 \epsilon_0 A}{d/2}\).
03

Computing the total capacitance

The total capacitance is the sum of the capacitances from each dielectric slab. However, we have to remember that these capacitances are in series, not in parallel. In series circuit, the total capacitance is given by the reciprocal of the sum of the reciprocals of the individual capacitances. Hence, the total capacitance \(C_{total}\) is given by: \(C_{total} = \frac{1} {(1/C_1)+(1/C_2)}\) Plugging in the expressions obtained in Step 2 and simplifying, one can find that \(C_{total} = \frac{(K_1 K_2) / (K_1 + K_2)}{\epsilon_0 A / d}\). This corresponds to answer choice (B).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Two thin wire rings each having a radius \(R\) are placed at a distance \(d\) apart with their axes coinciding. The charges on the two rings are \(+q\) and \(-q\). The potential difference between the centers of the two rings is $\ldots .$ (A) 0 (B) $\left.\left[\mathrm{q} /\left(2 \pi \epsilon_{0}\right)\right]\left[(1 / \mathrm{R})-\left\\{1 / \sqrt{(}^{2}+\mathrm{d}^{2}\right)\right\\}\right]$ (C) $\left[\mathrm{q} /\left(4 \pi \epsilon_{0}\right)\right]\left[(1 / \mathrm{R})-\left\\{1 / \sqrt{\left. \left.\left(\mathrm{R}^{2}+\mathrm{d}^{2}\right)\right\\}\right]}\right.\right.$ (D) \(\left[(q R) /\left(4 \pi \epsilon_{0} d^{2}\right)\right]\)

4 Points charges each \(+q\) is placed on the circumference of a circle of diameter \(2 \mathrm{~d}\) in such a way that they form a square. The potential at the centre is \(\ldots \ldots .\) (A) 0 (B) \((4 \mathrm{kd} / \mathrm{q})\) (C) \((\mathrm{kd} / 4 \mathrm{q})\) (D) \((4 \mathrm{kq} / \mathrm{d})\)

If electron in ground state of \(\mathrm{H}\) -atom is assumed in rest then dipole moment of electron proton system of \(\mathrm{H}\) -atom is $\ldots \ldots\( Orbit radius of \)\mathrm{H}\( atom in ground state is \)0.56 \AA$. (A) \(0.253 \times 10^{-29} \mathrm{~m}\) (B) \(0.848 \times 10^{-29} \mathrm{~m}\) (C) \(0.305 \times 10^{-29} \mathrm{~m}\) (D) \(1.205 \times 10^{-28} \mathrm{~m}\)

Three particles, each having a charge of \(10 \mu \mathrm{c}\) are placed at the corners of an equilateral triangle of side \(10 \mathrm{~cm}\). The electrostatic potential energy of the system is (Given $\left.\left[1 /\left(4 \pi \epsilon_{0}\right)\right]=9 \times 10^{9} \mathrm{~N} \cdot \mathrm{m}^{2} / \mathrm{c}^{2}\right)$ (A) \(100 \mathrm{~J}\) (B) \(27 \mathrm{~J}\) (C) Zero (D) Infinite

Two identical balls having like charges and placed at a certain distance apart repel each other with a certain force. They are brought in contact and then moved apart to a distance equal to half their initial separation. The force of repulsion between them increases \(4.5\) times in comparison with the initial value. The ratio of the initial charges of the balls is ....... (A) \(4: 1\) (B) \(6: 1\) (C) \(3: 1\) (D) \(2: 1\)

See all solutions

Recommended explanations on English Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free