Introduction to Electrodynamics · Problem 12.40

Electrodynamics and Relativity — David J. Griffiths

Physics · minkowski-force

Problem

Show that KμKμ=1−(u2/c2)cos⁡2θ1−u2/c2 F2,K_\mu K^\mu = \frac{1-(u^2/c^2)\cos^2\theta}{1-u^2/c^2}\,F^2, where θ\theta is the angle between u\mathbf{u} and F\mathbf{F}.

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