Kerr-Newman metric ($\Delta =r^2-2Mr+a^2+Q^2,a=J/M$)

The stationary axisymmetric Einstein–Maxwell family of asymptotically flat spacetimes extends the Kerr metric by including electric charge. Its horizon polynomial is the displayed $\Delta$; for $M^2>Q^2+a^2$ the roots are $r_{\pm }=M\pm \sqrt{M^2-Q^2-a^2}$. The outer Killing horizon has area $4\pi (r_{+}^2+a^2)$, angular velocity $a/(r_{+}^2+a^2)$ and electric potential $Q{r}_{+}/(r_{+}^2+a^2)$.

Differentiate $M=(r_{+}^2+a^2+Q^2)/(2r_{+})$, $J=Ma$ and $A=4\pi (r_{+}^2+a^2)$. Eliminating $d{r}_{+}$ and $da$ gives the displayed relation, with ${\Omega }_H=a/(r_{+}^2+a^2)$ and ${\Phi }_H=Q{r}_{+}/(r_{+}^2+a^2)$. Matching Hawking temperature to this First law of black-hole mechanics fixes the Bekenstein-Hawking entropy as $A/4$.

The outer-horizon surface gravity is $(r_{+}-r_{-})/(2(r_{+}^2+a^2))$. Hawking radiation or nondegenerate Euclidean black-hole regularity condition gives $T_H=\kappa /(2\pi )$ in units $G=\hslash =c=k_B=1$. The zero-temperature extremal value is the nonextremal limit; conical regularity alone does not fix a Euclidean period at a degenerate horizon.