Electrostatics

Coulomb's law, electric field, capacitors.

Coulomb's law

F = kq₁q₂/r²; superposition.

Electrostatics — Coulomb, field, potential, Gauss law
Notes

ELECTRIC CHARGE

  • Two types: positive, negative. Like repels, unlike attracts.
  • Quantized: q = ne (e = 1.6 × 10⁻¹⁹ C).
  • Conserved in isolated systems.
  • Additive (scalars).

COULOMB'S LAW

F = (1/4πε₀) · q₁q₂/r²

  • k = 1/(4πε₀) ≈ 9 × 10⁹ N·m²/C² (in vacuum).
  • In medium of permittivity ε: divide by εᵣ (dielectric constant).

ELECTRIC FIELD (E)

E = F/q₀ = (1/4πε₀)·Q/r² (point charge).

  • Vector field. Lines: from + to −, never cross.
  • Continuous charge distribution: dE = kdq/r².

Field of common charges:

  • Point charge: kQ/r².
  • Infinite line of charge: λ/(2πε₀r).
  • Infinite plane sheet: σ/(2ε₀).
  • Between parallel plates: σ/ε₀.
  • Dipole on axis (far): 2kp/r³; on equator: kp/r³.
  • Uniformly charged ring axis: kQx/(R²+x²)^(3/2).

ELECTRIC POTENTIAL (V)

V = work done per unit positive charge in bringing it from ∞ to that point.
V = (1/4πε₀)·Q/r (point charge).

  • Scalar — easier to handle.
  • E = −dV/dr (gradient).

Potential difference: V_A − V_B = W_AB/q.


ELECTRIC DIPOLE

  • Two equal and opposite charges separated by 2a.
  • Dipole moment: p = q · 2a, directed from −q to +q.
  • Torque in field: τ = p × E. (|τ| = pE sin θ.)
  • Potential energy: U = −p·E (= −pE cos θ).
  • Min U at θ = 0 (stable); max at θ = π (unstable).

GAUSS'S LAW

∮ E · dA = Q_enc / ε₀

Total electric flux through closed surface = (1/ε₀) × charge enclosed.

Applications (use symmetry):

  • Spherical shell: outside acts as point charge at center; inside E = 0.
  • Solid sphere of uniform charge: E_outside = kQ/r²; E_inside = kQr/R³.
  • Infinite line: E = λ/(2πε₀r).
  • Infinite plane sheet: E = σ/(2ε₀).
  • Spherical capacitor.

CONDUCTORS IN ELECTROSTATIC EQUILIBRIUM

  1. E = 0 inside conductor.
  2. Charge resides on surface.
  3. E just outside ⊥ surface, magnitude σ/ε₀.
  4. Potential constant inside and on surface.
  5. Sharp points have higher charge density (corona discharge).

CAPACITORS

C = Q/V.

  • Parallel plate (vacuum): C = ε₀A/d.
  • With dielectric: C = εᵣ ε₀ A/d.
  • Series: 1/C = 1/C₁ + 1/C₂ + ...
  • Parallel: C = C₁ + C₂ + ...
  • Energy: U = ½CV² = ½QV = Q²/2C.

Dielectric: insulator that polarizes in field. Reduces E inside → increases C.


EXAM HOOKS:

  • E from a uniformly charged sphere outside acts as if all charge at center.
  • For a conductor, inside E = 0 (always).
  • Gauss law: use symmetry (spherical/cylindrical/planar).
  • Force on dipole in uniform field = 0; torque ≠ 0.
  • Equipotential surfaces perpendicular to E at every point.

Capacitors

Q=CV, parallel plate, dielectrics.

Electrostatics — Coulomb, field, potential, Gauss law
Notes

ELECTRIC CHARGE

  • Two types: positive, negative. Like repels, unlike attracts.
  • Quantized: q = ne (e = 1.6 × 10⁻¹⁹ C).
  • Conserved in isolated systems.
  • Additive (scalars).

COULOMB'S LAW

F = (1/4πε₀) · q₁q₂/r²

  • k = 1/(4πε₀) ≈ 9 × 10⁹ N·m²/C² (in vacuum).
  • In medium of permittivity ε: divide by εᵣ (dielectric constant).

ELECTRIC FIELD (E)

E = F/q₀ = (1/4πε₀)·Q/r² (point charge).

  • Vector field. Lines: from + to −, never cross.
  • Continuous charge distribution: dE = kdq/r².

Field of common charges:

  • Point charge: kQ/r².
  • Infinite line of charge: λ/(2πε₀r).
  • Infinite plane sheet: σ/(2ε₀).
  • Between parallel plates: σ/ε₀.
  • Dipole on axis (far): 2kp/r³; on equator: kp/r³.
  • Uniformly charged ring axis: kQx/(R²+x²)^(3/2).

ELECTRIC POTENTIAL (V)

V = work done per unit positive charge in bringing it from ∞ to that point.
V = (1/4πε₀)·Q/r (point charge).

  • Scalar — easier to handle.
  • E = −dV/dr (gradient).

Potential difference: V_A − V_B = W_AB/q.


ELECTRIC DIPOLE

  • Two equal and opposite charges separated by 2a.
  • Dipole moment: p = q · 2a, directed from −q to +q.
  • Torque in field: τ = p × E. (|τ| = pE sin θ.)
  • Potential energy: U = −p·E (= −pE cos θ).
  • Min U at θ = 0 (stable); max at θ = π (unstable).

GAUSS'S LAW

∮ E · dA = Q_enc / ε₀

Total electric flux through closed surface = (1/ε₀) × charge enclosed.

Applications (use symmetry):

  • Spherical shell: outside acts as point charge at center; inside E = 0.
  • Solid sphere of uniform charge: E_outside = kQ/r²; E_inside = kQr/R³.
  • Infinite line: E = λ/(2πε₀r).
  • Infinite plane sheet: E = σ/(2ε₀).
  • Spherical capacitor.

CONDUCTORS IN ELECTROSTATIC EQUILIBRIUM

  1. E = 0 inside conductor.
  2. Charge resides on surface.
  3. E just outside ⊥ surface, magnitude σ/ε₀.
  4. Potential constant inside and on surface.
  5. Sharp points have higher charge density (corona discharge).

CAPACITORS

C = Q/V.

  • Parallel plate (vacuum): C = ε₀A/d.
  • With dielectric: C = εᵣ ε₀ A/d.
  • Series: 1/C = 1/C₁ + 1/C₂ + ...
  • Parallel: C = C₁ + C₂ + ...
  • Energy: U = ½CV² = ½QV = Q²/2C.

Dielectric: insulator that polarizes in field. Reduces E inside → increases C.


EXAM HOOKS:

  • E from a uniformly charged sphere outside acts as if all charge at center.
  • For a conductor, inside E = 0 (always).
  • Gauss law: use symmetry (spherical/cylindrical/planar).
  • Force on dipole in uniform field = 0; torque ≠ 0.
  • Equipotential surfaces perpendicular to E at every point.