Classical ElectrodynamicsProblems after each chapter |
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Page 141
... component of J means that A will have only a & component also . But this component A cannot be calculated by merely substituting J into ( 5.32 ) . Equation ( 5.32 ) holds only for rectangular components of A. * Thus we write rectangular ...
... component of J means that A will have only a & component also . But this component A cannot be calculated by merely substituting J into ( 5.32 ) . Equation ( 5.32 ) holds only for rectangular components of A. * Thus we write rectangular ...
Page 316
... component B , ( z ) of magnetic induction , as well as the z component Bo . • The continuity equation ( 10.1 ) reduces to V. v = 0 for an incompressible fluid . This is satisfied identically by a velocity in the x direction which ...
... component B , ( z ) of magnetic induction , as well as the z component Bo . • The continuity equation ( 10.1 ) reduces to V. v = 0 for an incompressible fluid . This is satisfied identically by a velocity in the x direction which ...
Page 476
... 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 approximate the radiation intensity by that due to the perpendicular ...
... 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 approximate the radiation intensity by that due to the perpendicular ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ