Rankers Physics
Topic: Capacitors
Subtopic: Parallel Plate Capacitor

Consider the arrangement of three plates X, Y and Z each of area A and separation d. The energy stored in the system when the plates are fully charged is: Image related to
\[\frac{\varepsilon_{0}AV^{2}}{2d}\]
\[\frac{\varepsilon_{0}AV^{2}}{d}\]
\[\frac{2\varepsilon_{0}AV^{2}}{d}\]
\[\frac{3\varepsilon_{0}AV^{2}}{2d}\]

Solution:

To solve for the energy stored in the system of three plates (X, Y, Z), let's break the system into simpler components:


1. System Description

  • The arrangement forms two capacitors:
    • Capacitor 1: Between plates X and Y.
    • Capacitor 2: Between plates Y and Z.
  • Each capacitor has the same plate area AA and plate separation dd.

The capacitance of a parallel plate capacitor is given by:

C=ε0AdC = \frac{\varepsilon_0 A}{d}

Thus, the capacitance of each capacitor is:

C1=C2=ε0AdC_1 = C_2 = \frac{\varepsilon_0 A}{d}


2. Effective Capacitance

The two capacitors are in parallel because plate Y is connected to the battery on one side and plate X and Z are on the opposite side. For capacitors in parallel, the effective capacitance is:

Ceq=C1+C2C_{\text{eq}} = C_1 + C_2 Ceq=ε0Ad+ε0Ad=2ε0AdC_{\text{eq}} = \frac{\varepsilon_0 A}{d} + \frac{\varepsilon_0 A}{d} = \frac{2 \varepsilon_0 A}{d}


3. Energy Stored in the System

The energy stored in a capacitor is:

U=12CeqV2U = \frac{1}{2} C_{\text{eq}} V^2

Substitute Ceq=2ε0AdC_{\text{eq}} = \frac{2 \varepsilon_0 A}{d}:

U=122ε0AdV2U = \frac{1}{2} \cdot \frac{2 \varepsilon_0 A}{d} \cdot V^2 U=ε0AV2dU = \frac{\varepsilon_0 A V^2}{d}


Final Answer:

The energy stored in the system is:

U=ε0AV2dU = \frac{\varepsilon_0 A V^2}{d}

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