Problem 4.96 — AC Circuit: Power in Pure Inductor and Capacitor

Problem Statement

Solve the capacitor/capacitance problem: Solve the capacitor/capacitance problem: Show that a pure inductor and a pure capacitor consume zero average power from an AC source. Pure inductor ($R=0$, $X_L = \omega L$): current lags voltage by $90°$, i.e., $\psi = -\pi/2$. $$\langle P_L\rangle = V_{\rm rms}I_{\rm rms}\cos(-\pi/2) = 0$$ Pure ca

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

$$\langle P_L\rangle = V_{\rm rms}I_{\rm rms}\cos(-\pi/2) = 0$$

$$C = \frac{\kappa\varepsilon_0 A}{d} = \frac{2\times8.85\times10^{-12}\times0.02}{10^{-3}} = \frac{3.54\times10^{-13}}{10^{-3}} = 3.54\times10^{-10}\,\text{F} = 354\,\text{pF}$$

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

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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