${\displaystyle \mathrm {T} \equiv \left({\boldsymbol {D))\otimes {\boldsymbol {E))-\mathrm {I} \int {\boldsymbol {D))\cdot d{\boldsymbol {E))\right)+\left({\boldsymbol {B))\otimes {\boldsymbol {H))-\mathrm {I} \int {\boldsymbol {B))\cdot d{\boldsymbol {H))\right)}$

${\displaystyle \mathrm {T} =\epsilon _{0}\left({\boldsymbol {E))\otimes {\boldsymbol {E))-\mathrm {I} \,{\frac ((\boldsymbol {E))^{2)){2))\right)+{\frac {1}{\mu _{0))}\left({\boldsymbol {B))\otimes {\boldsymbol {B))-\mathrm {I} \,{\frac ((\boldsymbol {B))^{2)){2))\right)}$

${\displaystyle {\begin{aligned}\nabla \cdot \mathrm {T} _{\text{e))&=\partial _{i}(D_{i}{\boldsymbol {E)))-D_{i}\nabla E_{i}\\&=(\partial _{i}D_{i}){\boldsymbol {E))+D_{i}\partial _{i}{\boldsymbol {E))-D_{i}\nabla E_{i}\\&=(\nabla \cdot {\boldsymbol {D))){\boldsymbol {E))+({\boldsymbol {D))\cdot \nabla _{E}){\boldsymbol {E))-\nabla _{E}({\boldsymbol {D))\cdot {\boldsymbol {E)))\\&=(\nabla \cdot {\boldsymbol {D))){\boldsymbol {E))-{\boldsymbol {D))\times (\nabla \times {\boldsymbol {E)))\\\end{aligned))}$

${\displaystyle {\boldsymbol {a))\times ({\boldsymbol {b))\times {\boldsymbol {c)))={\boldsymbol {b))({\boldsymbol {a))\cdot {\boldsymbol {c)))-({\boldsymbol {a))\cdot {\boldsymbol {b))){\boldsymbol {c))}$

${\displaystyle {\begin{aligned}\nabla \cdot \mathrm {T} &=(\nabla \cdot {\boldsymbol {D))){\boldsymbol {E))-{\boldsymbol {D))\times (\nabla \times {\boldsymbol {E)))+(\nabla \cdot {\boldsymbol {B))){\boldsymbol {H))-{\boldsymbol {B))\times (\nabla \times {\boldsymbol {H)))\\&=\rho {\boldsymbol {E))+{\boldsymbol {D))\times {\frac {\partial {\boldsymbol {B))}{\partial t))-{\boldsymbol {B))\times {\frac {\partial {\boldsymbol {D))}{\partial t))-{\boldsymbol {B))\times {\boldsymbol {j))\\&={\frac {\partial ({\boldsymbol {D))\times {\boldsymbol {B)))}{\partial t))+\rho {\boldsymbol {E))+{\boldsymbol {j))\times {\boldsymbol {B))\\\end{aligned))}$

${\displaystyle \oint _{\partial V}d{\boldsymbol {S))\cdot \mathrm {T} ={\frac {\partial }{\partial t))\int _{V}({\boldsymbol {D))\times {\boldsymbol {B)))dV+\int _{V}(\rho {\boldsymbol {E))+{\boldsymbol {j))\times {\boldsymbol {B)))dV}$

${\displaystyle {\boldsymbol {g))={\boldsymbol {D))\times {\boldsymbol {B))}$

${\displaystyle \{\lambda \}=\left\{-{\frac {\epsilon _{0}E^{2}+B^{2}/\mu _{0)){2)),~\pm {\sqrt {\left({\frac {\epsilon _{0}E^{2}-B^{2}/\mu _{0)){2))\right)^{2}+\left({\frac {\epsilon _{0)){\mu _{0))}{\boldsymbol {E))\cdot {\boldsymbol {B))\right)^{2))}\right\))$

${\displaystyle \{\lambda \}=\left\{-{\frac {\epsilon _{0}E^{2)){2)),~-{\frac {\epsilon _{0}E^{2)){2)),~+{\frac {\epsilon _{0}E^{2)){2))\right\))$

${\displaystyle \((\boldsymbol {v))\}=\left\((\boldsymbol {E))\times {\boldsymbol {E))_{y},~-{\boldsymbol {E))\times {\boldsymbol {E))_{z},~{\boldsymbol {E))E_{x}\right\))$