Electrodynamics II

Maxwell’s Equations in Differential Form:

  • Gauss’s Law for Electricity: ∇⋅E = ρ/ε₀
  • – Gauss’s Law for Magnetism: ∇⋅B = 0
  • – Faraday’s Law: ∇×E = -∂B/∂t
  • – Ampere-Maxwell Law: ∇×B = μ₀J + μ₀ε₀∂E/∂t

These four equations, together with the Lorentz force law F = q(E + v×B), completely describe classical electromagnetism.

Wave Equation: Maxwell’s equations lead to the electromagnetic wave equation: ∇²E = (1/c²)∂²E/∂t² and ∇²B = (1/c²)∂²B/∂t², where c = 1/√(μ₀ε₀) is the speed of light.

Properties of EM Waves: Electromagnetic waves are transverse waves with E and B fields perpendicular to each other and to the direction of propagation. They carry energy and momentum, with energy density u = ½(ε₀E² + B²/μ₀) and Poynting vector S = (1/μ₀)E×B describing energy flow.

μν, which combines E and B fields into a single mathematical object.