Classical ElectrodynamicsProblems after each chapter |
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Page 269
... dependence . It was shown in Chapter 6 that the solution for the vector potential A ( x , t ) in the Lorentz gauge is A ( x , t ) = d3x ' dt ' · Sar J ( x ' , t ' ) | x − x ' | + provided no boundary surfaces are present . assures the ...
... dependence . It was shown in Chapter 6 that the solution for the vector potential A ( x , t ) in the Lorentz gauge is A ( x , t ) = d3x ' dt ' · Sar J ( x ' , t ' ) | x − x ' | + provided no boundary surfaces are present . assures the ...
Page 296
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
Page 531
... dependence on atomic number as Z2 . So far we have considered the radiation which accompanies the disap- pearance of the charge of an orbital electron in the electron - capture process . An electron possesses a magnetic moment as well ...
... dependence on atomic number as Z2 . So far we have considered the radiation which accompanies the disap- pearance of the charge of an orbital electron in the electron - capture process . An electron possesses a magnetic moment as well ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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