Detailed Notes on Electromagnetic Theory and Waves

MAXWELL'S EQUATIONS
  • Gauss's Law:

    • E=Q<em>enclϵ</em>0\nabla \cdot \mathbf{E} = \frac{Q<em>{encl}}{\epsilon</em>0}

    • Relates electric field to charge density.

  • Gauss's Law for Magnetism:

    • B=0\nabla \cdot \mathbf{B} = 0

    • Indicates there are no magnetic monopoles.

  • Ampere's Law:

    • ×B=μ<em>0j+ϵ</em>0Et\nabla \times \mathbf{B} = \mu<em>0 \mathbf{j} + \epsilon</em>0 \frac{\partial \mathbf{E}}{\partial t}

    • Relates magnetic field to current density and changing electric field.

  • Faraday's Law:

    • ×E=Bt\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}

    • Indicates a changing magnetic field creates an electric field.

WAVE EQUATION
  • By manipulating Maxwell's Equations, we derive the wave equations for electric and magnetic fields:-

    • 2E(x,t)x2=μ<em>0ϵ</em>0c22E(x,t)t2\frac{\partial^2 E(x,t)}{\partial x^2} = \frac{\mu<em>0 \epsilon</em>0}{c^2} \frac{\partial^2 E(x,t)}{\partial t^2}

    • 2B(x,t)x2=μ<em>0ϵ</em>0c22B(x,t)t2\frac{\partial^2 B(x,t)}{\partial x^2} = \frac{\mu<em>0 \epsilon</em>0}{c^2} \frac{\partial^2 B(x,t)}{\partial t^2}

    • Where c=1μ<em>0ϵ</em>0c = \frac{1}{\sqrt{\mu<em>0 \epsilon</em>0}} is the speed of light.

ELECTROMAGNETIC WAVES
  • Intensity of light wave:

    • I=12ϵ<em>0cE</em>02I = \frac{1}{2} \epsilon<em>0 c E</em>0^2

  • The speed of electromagnetic waves:

    • c=1μ<em>0ϵ</em>0c = \frac{1}{\sqrt{\mu<em>0 \epsilon</em>0}}

INTERFERENCE and SUPERPOSITION PRINCIPLE
  • Constructive Interference: When waves are in-phase (Δϕ=0\Delta \phi = 0)

  • Destructive Interference: When waves are out-of-phase (Δϕ=π\Delta \phi = \pi)

DOUBLE-SLIT INTERFERENCE
  • Light waves passing through two closely spaced slits act as point sources, creating an interference pattern on the screen.

HUYGEN’S PRINCIPLE
  • Each point on a wavefront can be considered a source of secondary wavelets, expanding outwards.