]>
{ ∇ × B &vec; - 1 c &partial; E &vec; &partial; t = 4 π c j &vec; ∇ ċ E &vec; = 4 π ρ ∇ × E &vec; + 1 c &partial; B &vec; &partial; t = 0 &vec; ∇ ċ B &vec; = 0
R μ ν - 1 2 g μ ν R = 8 π G c 4 T μ ν