General Relativity: An Introduction for Physicists · Problem 6.1

Electromagnetism — Hobson, Efstathiou & Lasenby

Physics · maxwell-equations-tensor-form

Problem

Show that the second Maxwell equation in (6.7) can be written as ∂[σFμν]=0\partial_{[\sigma} F_{\mu\nu]} = 0.

Related theory

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