General Relativity: An Introduction for Physicists · Problem 6.5

Electromagnetism — Hobson, Efstathiou & Lasenby

Physics · lorentz-transformation-fields

Problem

Two Cartesian inertial frames SS and S′S' are in standard configuration. Show that the components of electric and magnetic fields in the two frames are related as follows: E′1=E1,B′1=B1,E'^1 = E^1, \qquad B'^1 = B^1, E′2=γ(E2−vB3),B′2=γ(B2+vc2E3),E'^2 = \gamma(E^2 - vB^3), \qquad B'^2 = \gamma\left(B^2 + \frac{v}{c^2}E^3\right), E′3=γ(E3+vB2),B′3=γ(B3−vc2E2).E'^3 = \gamma(E^3 + vB^2), \qquad B'^3 = \gamma\left(B^3 - \frac{v}{c^2}E^2\right). Show further that c2B⃗2−E⃗2c^2\vec{B}^2 - \vec{E}^2 is Lorentz invariant.

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