HC Verma Chapter 29 Problem 61 – Capacitance with Partial Dielectric (Side by Side)

Problem Statement

Solve the capacitor/capacitance problem: A parallel plate capacitor has plates of area $2A$ and separation $d$. The left half ($A$) is filled with dielectric $K_1$ and the right half ($A$) with dielectric $K_2$. Find the total capacitance. Two capacitors in parallel: $C = C_1 + C_2$ Step 1: $C_1 = K_1\varepsilon_0 A/d$ and $C_2 = K_2\varep

Given Information

  • See problem statement for all given quantities.

Physical Concepts & Formulas

Capacitors store electric charge on conducting plates separated by an insulator (dielectric). The capacitance $C = Q/V$ depends on geometry and dielectric constant. Energy stored is $U = Q^2/(2C) = CV^2/2 = QV/2$. Series and parallel combinations follow rules opposite to resistors.

  • $C = Q/V$ — definition of capacitance
  • $U = \frac{1}{2}CV^2 = \frac{Q^2}{2C}$ — energy stored
  • $C_{\text{parallel}} = C_1 + C_2$ — parallel combination
  • $1/C_{\text{series}} = 1/C_1 + 1/C_2$ — series combination
  • $C = \varepsilon_0\varepsilon_r A/d$ — parallel plate capacitor

Step-by-Step Solution

Step 1 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 2 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Step 3 — Verify the result: Check units, limiting cases, and order of magnitude to confirm the answer is physically reasonable.

Worked Calculation

Full substitution shown in the steps above.

Answer

$$\boxed{C = \dfrac{\kappa\varepsilon_0 A}{d}}$$

Physical Interpretation

Capacitors store energy in the electric field between their plates. Doubling the voltage quadruples the stored energy — an important design constraint for high-voltage applications. Charge sharing between capacitors is a lossless process only in the ideal case; real circuits dissipate energy in connecting resistance.


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