∮ E⃗ ⋅ dA⃗ = Qₑₙcₗₒₛₑd/ε₀
Electric flux through closed surface
∝ enclosed charge
E = kQ/r² (outside)
E = kQr/R³ (inside, uniform)
E = λ/2πε₀r
Cylindrical Gaussian surface
E = σ/2ε₀
Cylindrical Gaussian surface
V = W/q₀ = U/q₀
Work done per unit charge to bring from infinity
V = kQ/r (point charge)
Unit: Volt (V) = J/C
V_AB = V_A – V_B = W_AB/q₀
W = q₀(V_A – V_B)
Work done in moving charge from B to A
E⃗ = -∇V = -dV/dr r̂
E = -dV/dr (radial field)
For uniform field: E = V/d
⚡ Same potential everywhere on surface
🔄 No work needed to move charge along surface
⊥ Electric field always perpendicular to surface
V = V₁ + V₂ + V₃ + …
V = k∑(qᵢ/rᵢ)
Scalar addition (no vector addition needed)
V = (1/4πε₀) × (p⃗ ⋅ r̂)/r²
V = kp cos θ/r²
θ = angle between p⃗ and position vector
U = qV
U = kq₁q₂/r (two point charges)
U = (1/2)∑qᵢVᵢ (system of charges)
E = σ/ε₀
σ = local surface charge density
Field is perpendicular to surface
Permanent dipole moment
H₂O, HCl
Induced dipole moment
N₂, O₂, CO₂
K = ε/ε₀ = E₀/E
K > 1 for all dielectrics
C = Q/V
Ability to store charge per unit potential
Unit: Farad (F) = C/V
C = ε₀A/d (vacuum)
C = Kε₀A/d (with dielectric)
A = area of plates, d = separation
K = dielectric constant
Geometry | Capacitance Formula | Notes |
---|---|---|
Parallel Plates | C = ε₀A/d | Most common type |
Concentric Spheres | C = 4πε₀r₁r₂/(r₂-r₁) | r₁ < r₂ (radii) |
Isolated Sphere | C = 4πε₀R | R = radius |
Coaxial Cylinders | C = 2πε₀L/ln(b/a) | L = length, a < b |
1/C = 1/C₁ + 1/C₂ + …
Same charge, different voltages
C = C₁ + C₂ + …
Same voltage, different charges
U = ½CV² = ½QV = ½Q²/C
Energy density = ½ε₀E²
Energy stored in electric field
🔄 Moving belt transfers charge to metal dome
⚡ High voltage (up to millions of volts)
🛡️ Dome acts as Faraday cage
Constant | Symbol | Value | Unit |
---|---|---|---|
Coulomb’s constant | k | 9 × 10⁹ | Nm²/C² |
Permittivity of free space | ε₀ | 8.85 × 10⁻¹² | C²/Nm² |
Elementary charge | e | 1.6 × 10⁻¹⁹ | C |
Electron mass | mₑ | 9.1 × 10⁻³¹ | kg |
Proton mass | mₚ | 1.67 × 10⁻²⁷ | kg |
Understand field line concepts
Learn conductor properties
Practice Coulomb’s law problems
Capacitor combinations
Gauss’s law applications
E and V relationships
Van de Graaff generator
Electrostatic shielding
Understanding electrostatics is key to all electromagnetic phenomena!