Calculating Electromagnetic Field Energy Flux in Linear Medium

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Homework Help Overview

The discussion revolves around calculating the divergence of the energy flux vector \(\mathbf{S}\) in the context of electromagnetic fields within a linear medium characterized by permittivity \(\epsilon\) and permeability \(\mu\). The original poster is attempting to derive the expression for \(\nabla \cdot \mathbf{S}\) and is uncertain about the implications of their calculations.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster presents their calculations for \(\nabla \cdot \mathbf{S}\) and questions whether they have reached the correct result or if further simplifications are possible. Some participants suggest using known identities related to the electric and magnetic fields to simplify the expression further. Others mention the relevance of applying Gauss's Divergence theorem in future steps.

Discussion Status

The discussion is active, with participants providing guidance on potential simplifications and next steps. There is an exploration of different interpretations regarding the constants \(\epsilon\) and \(\mu\), indicating a lack of consensus on their assumed values in the problem context.

Contextual Notes

Participants are considering the assumptions about the material properties \(\epsilon\) and \(\mu\), questioning whether they are constants or variable in the general case. This reflects a broader inquiry into the problem's setup and the nature of the medium being analyzed.

cepheid
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Consider the electromagnetic field in a linear medium with material properties [itex]\epsilon \ \ \text{and} \ \ \mu[/itex]. Calculate [itex]\nabla \cdot \mathbf{S}[/itex] for the energy flux [itex]\mathbf{S = E \times H}[/itex].

My work:

[tex]\nabla \cdot \mathbf{S} = \nabla \cdot \frac{1}{\mu}(\mathbf{E \times B })[/tex]

[tex]= \frac{1}{\mu}[ \nabla \cdot(\mathbf{E \times B })][/tex]

[tex]= \frac{1}{\mu}[\mathbf{B} \cdot(\nabla \times \mathbf{E} }) - \mathbf{E} \cdot(\nabla \times \mathbf{B} }) ][/tex]

[tex]= \frac{1}{\mu}[\mathbf{B} \cdot(-\frac{\partial \mathbf{B}}{ \partial t}) - \mathbf{E} \cdot(\mu\epsilon\frac{\partial \mathbf{E}}{ \partial t})][/tex]

I guess my question is: is this the result? I have no idea what this problem wants. Are there at least any more immediately obvious simplifications?
 
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Almost there. Remember E . dE/dt = 1/2 d/dt |E|^2 and B . dB/dt = 1/2 d/dt |B|^2 (sorry I don't know Latex). Use these results in your last equation, and not surprisingly you should get the expression for the power per unit volume of the electric and magnetic fields.
 
That's the classic result for Del*S. A next step (in another assignment) would be derivation of the total flux of S through a closed surface enclosing charges and currents. That would utilize Gauss's Divergence theorem with your present result and other Maxwell's Equations.

[tex]\int\limits_{Surf}^{} \vec{S} * \vec{n} dA = \int\limits_{Vol}^{} \nabla*\vec{S} dV[/tex]

~
 
Last edited:
Thanks for all your help!
 
Are epsilon and mu constants??In the general case,they aren't,but i assume the problem asked for the simplest of them all.

Daniel.
 

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