Maxwell's Equations

]> Maxwell's Equations

Maxwell's Equations

${\begin{array}{rcl} \nabla \times B_{}^{\to} - \frac{1}{c} \frac{\partial E_{}^{\to}}{\partial t} & = & \frac{4 π}{c} j_{}^{\to} \\ \nabla ċ E_{}^{\to} & = & 4 π ρ \\ \nabla \times E_{}^{\to} + \frac{1}{c} \frac{\partial B_{}^{\to}}{\partial t} & = & 0_{}^{\to} \\ \nabla ċ B_{}^{\to} & = & 0 \end{array}$

Einstein's field equations

$R_{μ ν}^{} - \frac{1}{2} g_{μ ν}^{} R = \frac{8 π G}{c_{}^{4}} T_{μ ν}^{}$