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Page 367
... show that the time variables in K " and K ' are related by t " = t ' x ' c2 1 V. δν δν + v2 v2 v2 ( 11.50 ) 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 V. δν δν + v2 v2 v2 ( 11.50 ) correct to first order in dv . This shows that the direct transformation from K ' to K " involves an infinitesimal Lorentz ...
Page 371
... 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 x = - sin Y x3 + cos y X 4 ( 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 x = - sin Y x3 + cos y X 4 ( 11.77 ) Comparison of the coefficients in ( 11.77 ) ...
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... Show that the instantaneous power radiated per unit solid angle is : e2cẞ4 sin2 0 cos2 ( wt ' ) where B = awo / c . dP ( t ' ) = ΦΩ 4a2 ( 1 + ẞ cos 0 sin wot ' ) 5 ( b ) By performing a time averaging , show that the average power per ...
... Show that the instantaneous power radiated per unit solid angle is : e2cẞ4 sin2 0 cos2 ( wt ' ) where B = awo / c . dP ( t ' ) = ΦΩ 4a2 ( 1 + ẞ cos 0 sin wot ' ) 5 ( b ) By performing a time averaging , show that the average power per ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ