Electrostatics
Coulomb's law, electric field, capacitors.
Coulomb's law
F = kq₁q₂/r²; superposition.
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
- E = 0 inside conductor.
- Charge resides on surface.
- E just outside ⊥ surface, magnitude σ/ε₀.
- Potential constant inside and on surface.
- 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.
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
- E = 0 inside conductor.
- Charge resides on surface.
- E just outside ⊥ surface, magnitude σ/ε₀.
- Potential constant inside and on surface.
- 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.