Classical ElectrodynamicsProblems after each chapter |
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Page 189
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
Page 590
... electromagnetic structures of the neutron and proton . These have been explored by high - energy electron scattering , assuming that the electrons are point particles with no structure and that no changes occur in electro- dynamics at ...
... electromagnetic structures of the neutron and proton . These have been explored by high - energy electron scattering , assuming that the electrons are point particles with no structure and that no changes occur in electro- dynamics at ...
Page 621
... electromagnetic units in most common use today are the Gaussian and rationalized mks systems . The mks system has the virtue of overall convenience in practical , large - scale phenomena , especially in engineering applications . The ...
... electromagnetic units in most common use today are the Gaussian and rationalized mks systems . The mks system has the virtue of overall convenience in practical , large - scale phenomena , especially in engineering applications . The ...
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Common terms and phrases
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