Classical ElectrodynamicsProblems after each chapter |
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Page 367
... show that the time variables in K " and K ' are related by t " = t ' - x ' c2 1 1 δν δν + ( 11.50 ) v2 v2 correct to first order in dv . This shows that the direct transformation from K ' to K " involves an infinitesimal Lorentz ...
... show that the time variables in K " and K ' are related by t " = t ' - x ' c2 1 1 δν δν + ( 11.50 ) v2 v2 correct to first order in dv . This shows that the direct transformation from K ' to K " involves an infinitesimal Lorentz ...
Page 373
... shows a rotation of the axes through an angle y . The coordinates of the point P relative to the two sets of axes are related by X3 ' = cos y x3 + sin y x4 = -sin y x3 + cos Y X4 ( 11.77 ) Comparison of the coefficients in ( 11.77 ) ...
... shows a rotation of the axes through an angle y . The coordinates of the point P relative to the two sets of axes are related by X3 ' = cos y x3 + sin y x4 = -sin y x3 + cos Y X4 ( 11.77 ) Comparison of the coefficients in ( 11.77 ) ...
Page 501
... Show that the instantaneous power radiated per unit solid angle is : where ẞawo / c . dP ( t ' ) ΦΩ есва sin20 cos2 ( wt ' ) 4a2 ( 1 + cos 0 sin wot ́ ) 5 ( b ) By performing a time averaging , show that the average power per unit solid ...
... Show that the instantaneous power radiated per unit solid angle is : where ẞawo / c . dP ( t ' ) ΦΩ есва sin20 cos2 ( wt ' ) 4a2 ( 1 + cos 0 sin wot ́ ) 5 ( b ) By performing a time averaging , show that the average power per unit solid ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ