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{E~\nu }{(1+\nu )(1-2\nu )}}~;~~\mu ={\cfrac {E}{2(1+\nu )}}} The inverse relationship is ε = − ν E   tr ( σ )   1 + 1 + ν E   σ {\displaystyle {\boldsymbol...

{-{\frac {\mu }{2E}}}}\left(r_{+}^{2}-r_{-}^{2}\right)=\pi {\sqrt {-{\frac {\mu }{2E}}}}{\frac {GM\mu }{-E}}{\sqrt {\left({\frac {GM\mu }{E}}\right)^{2}+{\frac...

follows: g μ ν ( x ) = η a b   e μ a ( x ) e γ b ( x )   , {\displaystyle g_{\mu \nu }(x)=\eta _{ab}~e_{\mu }^{a}(x)e_{\gamma }^{b}(x)~,} with the general...

</math>T^{\mu \nu} r e p r e s e n t e d a s a l i n e a r c o m b i n a t i o n o f c o m p o n e n t s o f a r e a l [ [ . . / V e c t o r s / | v e c t o...

E = μ ( 3 λ + 2 μ ) λ + μ   ,       ν = λ 2 ( λ + μ ) {\displaystyle K=\lambda +{\frac {2}{3}}\mu ~,~~~E={\frac {\mu (3\lambda +2\mu )}{\lambda +\mu }}~...

_{C}{\vec {B}}\cdot \mathrm {d} {\vec {\ell }}&=\mu _{0}I+\epsilon _{0}\mu _{0}{\frac {\mathrm {d} \Phi _{E}}{\mathrm {d} t}}\end{aligned}}} See also http://ethw...

the equations: D = ε E {\displaystyle \mathbf {D} =\varepsilon \mathbf {E} } H = B / μ {\displaystyle \mathbf {H} =\mathbf {B} /\mu } where ε = ε r ε 0...

U={\vec {\mu }}\cdot {\vec {B}}} . Hall field = E = V / ℓ = B v d = I B n e A {\displaystyle E=V/\ell =Bv_{d}={\tfrac {IB}{neA}}} Lorentz force = q ( E → +...

∇ × E ) = − μ 0 ϵ 0 ∂ 2 E ∂ t 2 {\displaystyle \nabla \times (\nabla \times \mathbf {E} )=-\mu _{0}\epsilon _{0}{\frac {\partial ^{2}\mathbf {E} }{\partial...

  , {\displaystyle e_{\mu }^{a}(x)=\delta _{\mu }^{a}(x)+2\kappa \Phi _{\mu }^{a}(x)~,} where Φ μ a ( x ) {\displaystyle \Phi _{\mu }^{a}(x)} is small...

r}}} ▭ Biot–Savart law B → = μ 0 4 π ∫ w i r e I d ℓ → × r ^ r 2 {\displaystyle {\vec {B}}={\tfrac {\mu _{0}}{4\pi }}\int \limits _{wire}{\frac {Id{\vec...

divided in three categories that follow their massive partners, e , μ , τ {\displaystyle e,\,\mu \,,\tau } . All leptons (with the notable exceptions of all...

U={\vec {\mu }}\cdot {\vec {B}}} . Hall field = E = V / ℓ = B v d = I B n e A {\displaystyle E=V/\ell =Bv_{d}={\tfrac {IB}{neA}}} Lorentz force = q ( E → +...

{\displaystyle ~s_{\mu }={\frac {\rho _{0q}}{\rho _{0}}}A_{\mu }+D_{\mu }+U_{\mu }+\pi _{\mu }+\lambda _{\mu }+g_{\mu }+w_{\mu }.} By its meaning the...

{\ell }}=\mu _{0}\int _{S}({\vec {J}}+\epsilon _{0}{\frac {\partial {\vec {E}}}{\partial t}})\cdot d\mathbf {S} \,} where, ∫ S J → ⋅ d S = I e n c {\displaystyle...

_{\alpha \mu }J^{\mu }+F_{\alpha \mu }j^{\mu }+f_{\alpha \mu }J^{\mu }=-\nabla _{\mu }\left({U_{\alpha }}^{\mu }+{W_{\alpha }}^{\mu }+{P_{\alpha }}^{\mu }\right)...

3 ξ = ∂ ∂ ϕ η = − e μ β η     ;       σ 3 η = 0 {\displaystyle \sigma _{3\xi }={\frac {\partial }{\partial }}{\phi }{\eta }=-e\mu \beta \eta ~~;~~~\sigma...

L_{\text{solenoid}}\approx \mu _{0}N^{2}A\ell ,\,} L toroid ≈ μ 0 N 2 h 2 π ln ⁡ R 2 R 1 . {\displaystyle L_{\text{toroid}}\approx {\tfrac {\mu _{0}N^{2}h}{2\pi...

level is: Φ e = B S B = μ 0 e 4 π a B σ e = α 2 m e e σ e = α 2 Φ 0 ,   {\displaystyle \Phi _{e}=BS_{B}={\frac {\mu _{0}e}{4\pi a_{B}}}\sigma _{e}={\frac...

( θ , ϕ ) ) + V ( r ) } ψ ( r , θ , ϕ ) = E ψ ( r , θ , ϕ ) {\displaystyle \left\{-{\frac {\hbar ^{2}}{2\mu }}\left({\frac {\partial ^{2}}{\partial r^{2}}}+{\frac...