 Solution

Use coordinates $x^{\mu }=(ct,\mathbf{x})$, signature $(+---)$, and the convention $F^{0i}=-E_i/c$, $F^{ij}=-{ϵ}_{ijk}{B}_k$. The antisymmetric electromagnetic field tensor combines six field components:It transforms as $F^{\prime \mu \nu }={\Lambda }^{\mu }{}_{\alpha }{\Lambda }^{\nu }{}_{\beta }{F}^{\alpha \beta }$. Lowering indices changes the time–space signs: $F_{0i}=E_i/c$, while $F_{ij}=F^{ij}$. The covariant tensor instead uses the inverse coordinate Jacobian on each lower index.

For a frame moving with velocity $\mathbf{v}$ relative to the original one,Electric and magnetic fields therefore mix under a boost; they are frame-dependent parts of one tensor. For example, a purely transverse electric field acquires a magnetic field in a boosted frame. The electromagnetic field invariants $B^2-E^2/c^2$ and $\mathbf{E}\cdot \mathbf{B}$ restrict which fields can be eliminated by a frame change. The covariant force law $d{p}^{\mu }/d\tau =q{F}^{\mu }{}_{\nu }{U}^{\nu }$ guarantees consistent particle dynamics in all inertial frames.