Question

Derive the electromagnetic wave equation for equation and equation fields in vacuum starting from Maxwell's equations. Discuss the general properties of plane electromagnetic waves, including their speed and polarisation.

19 Jan 2026
Answer :
Word Count : 485
In classical electrodynamics, the behavior of electromagnetic fields in vacuum is governed by Maxwell's equations. In free space, where there are no charges or currents, these equations reduce to: [ \nabla \cdot \mathbf{E} = 0, \quad \nabla \cdot \mathbf{B} = 0, ] [ \nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}, \quad \nabla \times \mathbf{B} = \mu_0 \epsilon_0 \frac{\partial \mathbf{E}}{\partial t}. ] To derive the electromagnetic wave equation for the electric field (\mathbf{E}), we take the curl of Faraday’s law: [ \nabla \times (\nabla \times \mathbf{E}) = \nabla \times \left(-\frac{\partial \mathbf{B}}{\partial t}\right) = -\frac{\partial}{\partial t} (\nabla \times \mathbf{B}). ] Substituting Ampère’s law in vacuum (\nabla \times \mathbf{B} = \mu_0 \epsilon_0 \frac{\partial \mathbf{E}}{\partial t}), we obtain: [ \nabla \times (\nabla \times \mathbf{E}) = -\mu_0 \epsilon_0 \frac{\partial^2 \mathbf{E}}{\partial t^2}. ] Using the vector identity (\nabla \times (\nabla \times \mathbf{E})
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