Classical Electrodynamics |
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Page 367
Using the general formula (11.21) twice, it is a straightforward matter to show that
the time variables in K" and K" are related ... C c correct to first order in Öv. This
shows that the direct transformation from K' to K" involves an infinitesimal Lorentz
...
Using the general formula (11.21) twice, it is a straightforward matter to show that
the time variables in K" and K" are related ... C c correct to first order in Öv. This
shows that the direct transformation from K' to K" involves an infinitesimal Lorentz
...
Page 373
O £3 With definitions (11.68) and (11.70) it is elementary to show that (11.75)
yields exactly the Lorentz transformation ... + cos y 24 Comparison of the
coefficients in (11.77) with the transformation coefficients in (11.75) shows that
the angle p ...
O £3 With definitions (11.68) and (11.70) it is elementary to show that (11.75)
yields exactly the Lorentz transformation ... + cos y 24 Comparison of the
coefficients in (11.77) with the transformation coefficients in (11.75) shows that
the angle p ...
Page 501
(a) Show that the instantaneous power radiated per unit solid angle is: dP(t') e°cg
" sin” 0 cos” (ot') d.T T.47 (TTB coso sin of); where 3 = awolc. (b) By performing a
time averaging, show that the average power per unit solid angle is: dP e°cB4 T ...
(a) Show that the instantaneous power radiated per unit solid angle is: dP(t') e°cg
" sin” 0 cos” (ot') d.T T.47 (TTB coso sin of); where 3 = awolc. (b) By performing a
time averaging, show that the average power per unit solid angle is: dP e°cB4 T ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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