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Principles of Electromagnetism and Optics

Maxwell's Equations

Physics I 220 words Free to read

Four equations, and everything electrical, magnetic and optical follows — including the punchline hiding in the algebra: fields can chase each other through empty space at 1/μ0ε01/\sqrt{\mu_0\varepsilon_0}, which works out to the measured speed of light. Light is not like electromagnetism; it is electromagnetism.

Maxwell's four equations unify electricity, magnetism, and light.

E=ρε0(Gauss’s law for E)\nabla\cdot\vec{E} = \frac{\rho}{\varepsilon_0} \qquad\text{(Gauss's law for E)}

B=0(No magnetic monopoles)\nabla\cdot\vec{B} = 0 \qquad\text{(No magnetic monopoles)}

×E=Bt(Faraday’s law)\nabla\times\vec{E} = -\frac{\partial\vec{B}}{\partial t} \qquad\text{(Faraday's law)}

×B=μ0J+μ0ε0Et(Ampere-Maxwell)\nabla\times\vec{B} = \mu_0\vec{J} + \mu_0\varepsilon_0\frac{\partial\vec{E}}{\partial t} \qquad\text{(Ampere-Maxwell)}

Displacement current — Maxwell added ε0Et\varepsilon_0\dfrac{\partial\vec{E}}{\partial t} to Ampere's law. This term allows electromagnetic waves to exist in vacuum.

Electromagnetic waves — Maxwell's equations predict waves travelling at:

c=1μ0ε0=3.00×108  m/sc = \frac{1}{\sqrt{\mu_0\varepsilon_0}} = 3.00\times 10^8\;\text{m/s}

PropertyExpression
Speedc=fλc = f\lambda
E/BE/B ratioE=cBE = cB
Energy densityu=ε0E2=B2/μ0u = \varepsilon_0 E^{2} = B^{2}/\mu_0
Poynting vectorS=1μ0E×B\vec{S} = \dfrac{1}{\mu_0}\vec{E}\times\vec{B}
Key insight: Maxwell showed that light is an electromagnetic wave. This unified optics with electromagnetism — one of the greatest achievements in physics.
Common pitfall: An electromagnetic wave needs no medium — the fields sustain each other. The EE and BB fields are in phase, mutually perpendicular, and both perpendicular to the travel direction; a common error is drawing them out of phase like energy-trading oscillators.

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Principles of Electromagnetism and Optics