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AP® Physics C: Electricity and Magnetism · Unit 10 · Topic 10.1

Electrostatics with Conductors: Revision Notes (Physics C: E&M 10.1)

One-page recap of conductors in electrostatic equilibrium: zero interior field, surface charge, equipotentials, E = σ/ε₀, sharp points, polarization, cavities and shielding.

Short on time? This page is the recap. For the reasoning, Figure 1 and the worked examples, use the full study guide. This topic is part of the calculus-based course.

Recap

  • An ideal conductor has electrons that move freely. Positive net charge means missing electrons, modelled as positive carriers on the surface.
  • Free charges move until the field inside cancels. This electrostatic equilibrium is reached effectively at once.
  • E = 0 inside the metal → by Gauss’s law, no net charge inside → all excess charge is on the surface.
  • E = 0 inside → ΔV = −∫E·dl = 0 → the whole conductor, surface included, is one equipotential.
  • The field just outside is perpendicular to the surface, with E = σ/ε₀.
  • σ is greatest at points and edges, so the field is strongest there.
  • In an external field, a conductor polarizes: induced − and + charges appear on opposite sides, the net charge stays the same, and the inside stays field-free.
  • A closed conducting shell shields its cavity from outside fields.

Key relationships

Situation Result
Inside the metal of any conductor in equilibrium E = 0; V = constant
Just outside a conducting surface E = σ/ε₀, perpendicular to the surface
Thin isolated sheet (for comparison) E = σ/(2ε₀)
Isolated conducting sphere, charge Q σ = Q/(4πR²); E = Q/(4πε₀r²) for r ≥ R; E = 0 inside
Empty cavity in a conductor no charge on the wall; E = 0 in the cavity
Charge q in a cavity of a conductor with net charge Q wall: −q; outer surface: Q + q

Assumptions

  • Electrostatic equilibrium: no charge is moving.
  • “Ideal” conductor: charges move freely; insulators behave differently.
  • Spherical results need spherical symmetry and no nearby charges.

Mistakes to avoid

  1. V = 0 inside because E = 0. V is constant, not zero.
  2. σ/(2ε₀) next to a conductor. It is σ/ε₀.
  3. Charge −q on the outer surface. The induced −q is on the cavity wall.
  4. Uniform σ on every shape. Only an isolated sphere has uniform σ.
  5. “Shielding works both ways.” A charge inside still produces a field outside unless the shell is grounded.

Quick self-check

  1. Just outside a conductor, σ = 4.0 × 10⁻⁸ C/m². What is E? (4.5 × 10³ N/C, perpendicular to the surface)
  2. +2.0 nC is placed in the cavity of a neutral metal shell. What are the charges on the inner and outer surfaces? (−2.0 nC and +2.0 nC)
  3. A metal sphere is at 500 V. What is the potential at its centre? (500 V)
  4. A closed, neutral metal box stands in a uniform external field of 5.0 × 10³ N/C. What is E in the empty space inside? (Zero: charges induced on the outer surface cancel the outside field everywhere within it)

Next: practice questions.

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