Classical ElectrodynamicsProblems after each chapter |
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Page 151
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
... atomic electrons possess intrinsic magnetic moments which cannot be expressed in terms of a current density . These moments can give rise to dipole fields which vary appreciably on the atomic scale of dimensions . To treat these atomic ...
Page 368
... atomic electron . In atomic nuclei the nucleons experience strong accelerations due to the specifically nuclear forces . The electromagnetic forces are comparatively weak . In an approximate way one can treat the nucleons as moving ...
... atomic electron . In atomic nuclei the nucleons experience strong accelerations due to the specifically nuclear forces . The electromagnetic forces are comparatively weak . In an approximate way one can treat the nucleons as moving ...
Page 559
... atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of the same frequency is ...
... atomic or nuclear transition the lowest nonvanishing multipole will generally be the only one of importance . The ratio of transition probabilities for successive orders of either electric or magnetic multipoles of the same frequency is ...
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