Question: (a) Carry through the argument in Sect. 8.1.2, starting with Eq. 8.6, but using Jf in place of J. Show that the Poynting vector becomes

(a) Carry through the argument in Sect. 8.1.2, starting with Eq. 8.6, but using Jf in place of J. Show that the Poynting vector becomes S = E x H, and the rate of change of the energy density in the fields is For linear media, show that

(b) In the same spirit, reproduce the argument in Sect. 8.2.2, starting with Eq. 8.15, with, p f and Jf in place of p and J. Don't bother to construct the Maxwell stress tensor, but do show that the momentum density is

31 lem = Part (a) S = Ex H, D t Part

31 lem = Part (a) S = Ex H, D t Part (b) (E.D + B.H). 2 = D x B. = E. t +H

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a If were only interested in the work done on free charges and currents Eq 86 becomes dW Eq 755 so E... View full answer

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