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

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SUMMARY

The discussion focuses on the role of J in Dynamic Ohm's Law, specifically its relationship to Ampère's Law. J is defined as the sum of J_m (magnetization current), J_f (free current), and the time derivative of polarization (∂_t P). The equations presented clarify that J in dynamic scenarios incorporates both free and magnetization currents, aligning with the principles of electromagnetism as described by Maxwell's equations.

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  • Understanding of Ampère's Law and its applications
  • Familiarity with Maxwell's equations
  • Knowledge of electric polarization (P) and magnetization (M)
  • Basic concepts of dynamic versus static electric fields
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  • Study the derivation and implications of Maxwell's equations in electromagnetism
  • Explore the relationship between electric fields and current density in dynamic systems
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  • Learn about the applications of dynamic Ohm's Law in electrical engineering
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Students of physics, electrical engineers, and researchers focusing on electromagnetism and its applications in dynamic systems.

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Homework Statement


What is J in Ohms law in dynamics?

Homework Equations


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

The Attempt at a Solution


Is J = J_m + J_f + \partial_t (P) ?
 
Last edited:
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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).
 

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