Classical Electrodynamics |
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Page 248
E x H+ 8.47)* 4tr_l 2 ( ) (8.47) whose real part gives the time-averaged flux of
energy. For the two types of field we find, using (8.24): 2 ok levor + i; ww. S = ± (
8.48) 8try 1 2 - y” # =|es IV,ws" — i – p"V,"p Au k where the upper (lower) line is
for TM ...
E x H+ 8.47)* 4tr_l 2 ( ) (8.47) whose real part gives the time-averaged flux of
energy. For the two types of field we find, using (8.24): 2 ok levor + i; ww. S = ± (
8.48) 8try 1 2 - y” # =|es IV,ws" — i – p"V,"p Au k where the upper (lower) line is
for TM ...
Page 273
... one of which gives a transverse magnetic induction and the other of which
gives a transverse electric field. These physically distinct contributions can be
separated. Fig. 9.1 Short, center-fed, linear antenna. x -#. [Sect. 9.3] Simple
Radiating ...
... one of which gives a transverse magnetic induction and the other of which
gives a transverse electric field. These physically distinct contributions can be
separated. Fig. 9.1 Short, center-fed, linear antenna. x -#. [Sect. 9.3] Simple
Radiating ...
Page
Bohr's formula (13.36) gives a reasonable description of the energy loss of
relatively slow alpha particles and heavier nuclei. But for electrons, mesons,
protons, and even fast alphas, it overestimates the energy loss considerably. The
reason is ...
Bohr's formula (13.36) gives a reasonable description of the energy loss of
relatively slow alpha particles and heavier nuclei. But for electrons, mesons,
protons, and even fast alphas, it overestimates the energy loss considerably. The
reason is ...
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Contents
Introduction to Electrostatics | 1 |
Nș 3 | 3 |
Greens theorem | 14 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |