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AP® Physics C: Electricity and Magnetism · Unit 8 · Topic 8.6

Gauss's Law: Revision Notes (Physics C: E&M 8.6)

One-page recap of Gauss's law for the calculus-based course: Gaussian surfaces, standard field results, integrating non-uniform densities and the limit checks.

Short on time? This page is the recap. For the derivations, Figure 1 and the worked examples, use the full study guide. This topic is in the calculus-based course only; it is not part of Physics 2.

Recap

  • Gauss’s law links the net flux through a closed surface to the net charge inside it. Area vectors point outward.
  • The flux does not change if you resize the surface, as long as q_enc stays the same.
  • The law is always true, but it gives E directly only when symmetry makes E constant and perpendicular on parts of the surface, and parallel (zero flux) on the rest.
  • The course applies it quantitatively to point charges and to spherical, cylindrical and planar symmetry.
  • ε₀ = 8.85 × 10⁻¹² C²/(N·m²); 1/(4πε₀) = 8.99 × 10⁹ N·m²/C².

Key relationships

Charge distribution Gaussian surface Field
Point charge or outside any spherical distribution sphere, radius r E = Q/(4πε₀r²)
Inside a uniform solid sphere (r < R) sphere, radius r E = Qr/(4πε₀R³) = ρr/(3ε₀)
Infinite line, charge per length λ coaxial cylinder E = λ/(2πε₀r)
Inside a uniform long cylinder (r < R) coaxial cylinder E = ρr/(2ε₀)
Infinite thin sheet, σ pillbox E = σ/(2ε₀), independent of distance
Non-uniform sphere, ρ(r) sphere, radius r q_enc = ∫₀ʳ ρ(r′)4πr′² dr′, then E = q_enc/(4πε₀r²)

Assumptions behind the results

  • The charge distribution has exact symmetry: “infinite” lines and sheets, and perfect spheres.
  • Insulators hold their charge in place; conductors are treated in Unit 10.
  • The system is in electrostatic equilibrium (charges at rest).

Mistakes to avoid

  1. Using total Q inside a body. Use q_enc(r).
  2. ρ × volume when ρ varies. Integrate ρ dV.
  3. Zero flux ⇒ zero field. Wrong: zero flux means zero enclosed charge.
  4. End caps on a line-charge cylinder. They carry no flux.
  5. σ/ε₀ for a thin sheet. Two faces of the pillbox carry flux, so E = σ/(2ε₀).
  6. Skipping the checks. E should match at r = R and approach Q/(4πε₀r²) for large r.

Quick self-check

  1. What is the net flux through a closed surface around +8.85 × 10⁻¹² C? (1.00 N·m²/C)
  2. Inside a uniform sphere, how does E change if r is doubled (still inside)? (It doubles, since E ∝ r)
  3. A sphere has ρ = ρ₀r/R. What is q_enc(r)? (πρ₀r⁴/R)

Next: practice questions.

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