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Potential Energy of a Charged Conductor

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Estimated time: 5 minutes
CISCE: Class 12

Introduction

When a conductor is charged, external work must be done to bring charge onto it against the repulsive force of the charge already present. This work is stored as electrostatic potential energy in the conductor.ncert

CISCE: Class 12

Derivation

Step 1: Instantaneous potential:
At any stage of charging, if the conductor carries charge q, its potential is:

  • V = \[\frac {q}{C}\]

Step 2: Work for an infinitesimal charge increment:
Bringing an additional small charge dq from infinity requires work:

  • dW = V dq = \[\frac {q}{C}\] dq

Step 3: Integrate over the full charging process:
Total work done in charging the conductor from 0 to final charge Q:

  • W = \[\int_0^Q\frac{q}{C}dq=\frac{Q^2}{2C}\]

Step 4: Energy stored equals work done:

  • U = \[\frac {Q^2}{2C}\]

Step 5: Alternate forms using Q = CV:

  • U = \[\frac {1}{2}\]CV2 = \[\frac {1}{2}\]QV
CISCE: Class 12

Graphical Representation

  • Graph 1: U vs Q — A parabola opening upward passing through the origin (since U ∝ Q2); label axes as Charge (Q) on the x-axis and Energy (U) on the y-axis.

  • Graph 2: U vs V — A parabola opening upward passing through the origin (since U ∝ V2); label axes as Potential (V) on the x-axis and Energy (U) on the y-axis.
CISCE: Class 12

Real-Life Connection

Capacitors storing energy via this same principle are used in camera flash units, defibrillators, and power backup circuits, where rapid release of stored electrostatic energy is required.

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