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
Escape velocity extremal solution
v e = 2 G M r − G 2 M 2 c 2 r 2