Classical ElectrodynamicsProblems after each chapter |
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... perpendicular to the orthogonal vectors E and B , u = c ( Ex B ) B2 ( 12.98 ) we find the fields in K ' to be E1 ' = 0 , E1 ' = YE + × B = 0 ( 12.99 ) 1 B2 B = 0 , γ B2 B = B = ( ) B In the frame K ' the only field acting is a static ...
... perpendicular to the orthogonal vectors E and B , u = c ( Ex B ) B2 ( 12.98 ) we find the fields in K ' to be E1 ' = 0 , E1 ' = YE + × B = 0 ( 12.99 ) 1 B2 B = 0 , γ B2 B = B = ( ) B In the frame K ' the only field acting is a static ...
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John David Jackson. parallel to and perpendicular to the velocity . But we have just seen that for comparable parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that ...
John David Jackson. parallel to and perpendicular to the velocity . But we have just seen that for comparable parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that ...
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... perpendicular to the plane containing ß , and n . The direction of polarization of the radiation is given by the vector nx ( n x Aẞ ) . This is perpendicular to n ( as it must be ) and can be resolved into components along and Thus nx ...
... perpendicular to the plane containing ß , and n . The direction of polarization of the radiation is given by the vector nx ( n x Aẞ ) . This is perpendicular to n ( as it must be ) and can be resolved into components along and Thus nx ...
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