Reissner-Nordström

Kerr

Kerr-Newman

Horizon

r h = G M c 2 ± G 2 M 2 c 4 r Q 2

r h = G M c 2 ± G 2 M 2 c 4 a 2

r h = G M c 2 ± G 2 M 2 c 4 r Q 2 a 2

Extremal solution

r Q = G M c 2

a = G M c 2

r Q 2 + a 2 = G 2 M 2 c 4

Extremal solution horizon

r h = G M c 2

r h = G M c 2

r h = G M c 2

Escape velocity extremal solution

v e = 2 G M r G 2 M 2 c 2 r 2

v e = 2 G M r G 2 M 2 c 2 r 2

v e = 2 G M r G 2 M 2 c 2 r 2