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Physics · Ch 8 — Electromagnetic Waves

Electromagnetic Waves

8.3

Electromagnetic Waves

What Are Electromagnetic Waves?

Electromagnetic waves are self-sustaining oscillations of electric and magnetic fields that travel through space at the speed of light. They are produced by accelerating charges and do not require a medium — they can propagate through vacuum.

The key idea: a changing electric field generates a magnetic field, and a changing magnetic field generates an electric field. This mutual induction allows the wave to move forward.


Derivation from Maxwell’s Equations (Conceptual)

In a region with no charges (ρ=0\rho = 0) and no currents (J=0\mathbf{J} = 0), Maxwell’s equations in vacuum become:

  • ∇⋅E=0\nabla \cdot \mathbf{E} = 0
  • ∇⋅B=0\nabla \cdot \mathbf{B} = 0
  • ∇×E=−∂B∂t\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}
  • ∇×B=μ0ε0∂E∂t\nabla \times \mathbf{B} = \mu_0 \varepsilon_0 \frac{\partial \mathbf{E}}{\partial t}

Taking the curl of Faraday’s law and using the vector identity ∇×(∇×E)=∇(∇⋅E)−∇2E\nabla \times (\nabla \times \mathbf{E}) = \nabla(\nabla \cdot \mathbf{E}) - \nabla^2 \mathbf{E}, with ∇⋅E=0\nabla \cdot \mathbf{E} = 0, we get:

∇2E=μ0ε0∂2E∂t2\nabla^2 \mathbf{E} = \mu_0 \varepsilon_0 \frac{\partial^2 \mathbf{E}}{\partial t^2}

This is the wave equation for E\mathbf{E}. A similar equation holds for B\mathbf{B}:

∇2B=μ0ε0∂2B∂t2\nabla^2 \mathbf{B} = \mu_0 \varepsilon_0 \frac{\partial^2 \mathbf{B}}{\partial t^2}

Comparing with the standard wave equation ∇2f=1v2∂2f∂t2\nabla^2 f = \frac{1}{v^2} \frac{\partial^2 f}{\partial t^2}, the wave speed is:

c=1μ0ε0c = \frac{1}{\sqrt{\mu_0 \varepsilon_0}}

where:

  • μ0=4π×10−7 N/A2\mu_0 = 4\pi \times 10^{-7} \, \text{N/A}^2 (permeability of free space)
  • ε0=8.85×10−12 C2/N⋅m2\varepsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2/\text{N·m}^2 (permittivity of free space)

Plugging in the numbers gives c≈3.00×108 m/sc \approx 3.00 \times 10^8 \, \text{m/s} — the speed of light in vacuum.


Properties of Electromagnetic Waves

  • Transverse nature: Both E\mathbf{E} and B\mathbf{B} are perpendicular to the direction of propagation.
  • Mutually perpendicular: E\mathbf{E} and B\mathbf{B} are perpendicular to each other.
  • In phase: The electric and magnetic fields oscillate in phase — they reach maxima and minima together.
  • Relation between field magnitudes: At any point and time,

EB=c\frac{E}{B} = c

where EE and BB are the instantaneous magnitudes of the electric and magnetic fields.

  • Energy transport: Electromagnetic waves carry energy. The energy per unit volume (energy density) is: …