Մասնակից:Vahram Mekhitarian/Ավազարկղ/Բանաձևեր

$\oint _{L}\mathbf {F} _{I}\cdot d\mathbf {L} =-{\frac {1}{c}}{\frac {d}{dt}}\iint _{S}\mathbf {B} \cdot d\mathbf {S}$

${\begin{bmatrix}c\,t'\\x'\\y'\\z'\end{bmatrix}}=\left({\begin{bmatrix}1\ &0\ &0\ &0\\0\ &1\ &0\ &0\\0\ &0\ &1\ &0\\0\ &0\ &0\ &1\\\end{bmatrix}}+\gamma {\begin{bmatrix}0\ &\beta _{x}\ &\beta _{y}\ &\beta _{z}\\\beta _{x}\ &0\ &0\ &0\\\beta _{y}\ &0\ &0\ &0\\\beta _{z}\ &0\ &0\ &0\\\end{bmatrix}}+(\gamma -1){\begin{bmatrix}1\ &0\ &0\ &0\\0\ &{\beta _{x}^{2}}/{\beta ^{2}}&{\beta _{x}\beta _{y}}/{\beta ^{2}}&{\beta _{x}\beta _{z}}/{\beta ^{2}}\\0\ &{\beta _{y}\beta _{x}}/{\beta ^{2}}&{\beta _{y}^{2}}/{\beta ^{2}}&{\beta _{y}\beta _{z}}/{\beta ^{2}}\\0\ &{\beta _{z}\beta _{x}}/{\beta ^{2}}&{\beta _{z}\beta _{y}}/{\beta ^{2}}&{\beta _{z}^{2}}/{\beta ^{2}}\\\end{bmatrix}}\right){\begin{bmatrix}c\,t\\x\\y\\z\end{bmatrix}}$

The Faraday Law of Induction for an Arbitrarily Moving Charge