What is the Role of J in Dynamic Ohm's Law?

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berra
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Homework Statement


What is J in Ohms law in dynamics?

Homework Equations


Ampères law:
[tex]\nabla \times H = J_f + \partial_t D = J_f + \partial_t ( \epsilon_0 E + P)[/tex]
[tex]\nabla \times H = \nabla \times (\mu_0^{-1} B - M) = \nabla \times (\mu_0^{-1} B) - \nabla \times (M) = \nabla \times (\mu_0^{-1} B) - J_m[/tex]
[tex]\nabla \times (\mu_0^{-1} B) = J_m + J_f + \partial_t ( \epsilon_0 E + P)[/tex]
Ohms law (statics?):
[tex]\sigma E = J[/tex]
Relation between J and p (magnetostatics ?):
[tex]\int_V{ J dV} = \frac{dp}{dt} = \frac{d\int_{V'}{r' \rho{r'} dV'}}{dt}[/tex]

The Attempt at a Solution


Is [itex]J = J_m + J_f + \partial_t (P)[/itex] ?
 
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I think J in Ohms law in dynamics is the same as the J in Ampères law in statics, which is equal to J_m + J_f + \partial_t (P).