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Permittivity of free space (ε0)
8.854×10⁻¹² C²N⁻¹m⁻² — represents the resistance encountered forming an E-field in vacuum
Electric field (E) definition
Force per unit charge; units N/C or V/m
Equipotential lines
Lines/surfaces of constant potential V. The E-field is always perpendicular to them. Work moving a charge along one is ZERO
Electric potential φ (or V)
Work done per unit charge moving a test charge from infinity to a point. E = −∇φ, with V(∞)=0 by convention
Total charge from volume charge density
Q = ∭ρ dτ, where ρ is volume charge density (C/m³)
Total charge from surface charge density
Q = ∬σ da, where σ is surface charge density (C/m²). For a homogeneous disk: Q = σπR²
Electric field, superposition of point charges
E = (1/4πε0)·Σ(qi/ri²)·r̂i
Electric flux (ΦE)
A measure of the number of field lines passing through a surface
Electric flux formula
ΦE = ∬E·da. For a uniform field: ΦE = EA·cosθ
Gauss's Law (integral form)
∮E·da = Q(enclosed)/ε0 — depends ONLY on the net enclosed charge, never on the surface's shape or size
Gauss's Law (differential form)
∇·E = ρ/ε0
Electric dipole moment (p)
p = qd, the product of charge magnitude q and separation distance d. Units: C·m
Electrostatic energy — discrete charges
U = ½ Σ(i≠j) (1/4πε0)(qiqj/rij)
Electrostatic energy — continuous charge distribution
U = ½∫ρφ dV
Magnetic field (B) / magnetic flux density
Units: Tesla (T)
Current density (j)
Current per unit area. Units: A/m²
Vacuum permeability (μ0)
4π×10⁻⁷ N/A² — constant for vacuum's ability to support magnetic fields
Ampère's Law (integral form)
∮B·dl = μ0·I(enclosed)
Ampère's Law (differential form)
∇×B = μ0·j
Vector potential (A)
B = ∇×A, using the Coulomb gauge ∇·A = 0
Magnetic flux (ΦB)
Total magnetic field through an area. Units: Weber (Wb). ΦB = ∬B·dA
EMF (electromotive force)
NOT a force — the work done per unit charge to maintain current. Units: Volts. EMF = ∮E·dl
Faraday's Law
EMF = −dΦB/dt
Lenz's Law
Induced current flows so as to oppose the change in flux that created it — the minus sign in Faraday's law
Displacement current
Maxwell's correction to Ampère's Law: a changing E-field also generates a B-field. I_d = ε0·(dΦE/dt)
Ampère-Maxwell Law
∇×B = μ0j + μ0ε0(∂E/∂t)