Classical ElectrodynamicsProblems after each chapter |
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Page 427
... parallel to the x axis ; B is parallel to the y axis . ( a ) For | E | < | B | make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory . ( b ) Repeat ...
... parallel to the x axis ; B is parallel to the y axis . ( a ) For | E | < | B | make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory . ( b ) Repeat ...
Page 475
... parallel to the velocity ( 14.43 ) or ( 14.27 ) with the power radiated for acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion , the magnitude of the rate of change of ...
... parallel to the velocity ( 14.43 ) or ( 14.27 ) with the power radiated for acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion , the magnitude of the rate of change of ...
Page 476
... parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and ...
... parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ