⚡ Physics — Class XII

Electrostatic Potential and Capacitance

How energy is stored in electric fields and the devices that store charge

📖 Chapter 2 ⏱ ~60 min read 🏷️ Electrostatics

Table of Contents

  1. Introduction
  2. Electric Potential
  3. Potential due to a Point Charge
  4. Potential due to a Dipole
  5. Equipotential Surfaces
  6. Capacitance
  7. Parallel Plate Capacitor
  8. Capacitors in Series and Parallel
  9. Energy Stored in a Capacitor

2.1 Introduction

In previous chapters, we studied the notion of potential energy and the work-energy theorem. In this chapter, we extend these ideas to electric charges. The concept of electric potential energy and electric potential helps us understand how energy is stored in electric fields and how capacitors work.

2.2 Electric Potential

The electric potential at a point is the work done per unit positive charge in bringing a test charge from infinity to that point without acceleration:

V = W/q₀
Unit: Volt (V) = 1 J/C. Scalar quantity. V is positive near positive charges, negative near negative charges.

2.3 Potential due to a Point Charge

V = kq/r
V is inversely proportional to r (not r² like E). At infinity, V = 0 by convention.
Potential and capacitance
Figure 2.1 — Electric potential around a point charge, parallel plate capacitor, and key concepts

2.4 Potential due to a Dipole

For an electric dipole with charges ±q separated by distance 2a:

V = kp cos θ / r²
p = qa (dipole moment). At equatorial plane (θ = 90°), V = 0. Along axis (θ = 0°), V = kp/r².

2.5 Equipotential Surfaces

Surfaces where the potential is the same at every point. Key properties:

2.6 Capacitance

Capacitance is the ability of a system to store charge per unit potential difference:

C = Q/V
Unit: Farad (F) = 1 C/V. 1 μF = 10⁻⁶ F, 1 pF = 10⁻¹² F. Capacitance depends on geometry and dielectric.

2.7 Parallel Plate Capacitor

The most common capacitor: two parallel conducting plates separated by distance d:

C = ε₀A/d
A = area of plates, d = separation. With dielectric: C = κε₀A/d, where κ = dielectric constant (> 1).
💡 Dielectric Effect

Inserting a dielectric (insulator) between plates increases capacitance by factor κ. The dielectric gets polarized, creating an internal field that opposes the external field, reducing net field and allowing more charge storage.

2.8 Capacitors in Series and Parallel

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Series Combination

1/C = 1/C₁ + 1/C₂ + ...
Total capacitance is less than smallest. Same charge on each, voltages add.

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Parallel Combination

C = C₁ + C₂ + ...
Total capacitance is sum of all. Same voltage across each, charges add.

2.9 Energy Stored in a Capacitor

U = ½CV² = ½Q²/C = ½QV
Energy is stored in the electric field between plates. Energy density: u = ½ε₀E²
⚠️ Energy in Electric Field

The energy is not stored on the plates but in the electric field between them. The energy density (energy per unit volume) is u = ½ε₀E², showing that stronger fields store more energy.

Ch 1 — Electric Charges and Fields Ch 3 — Current Electricity