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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?
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?