Classical ElectrodynamicsProblems after each chapter |
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Page 145
... Distribution ; Magnetic Moment We now consider the properties of a general current distribution which is localized in a small region of space , " small " being relative to the scale of length of interest to the observer . The proper ...
... Distribution ; Magnetic Moment We now consider the properties of a general current distribution which is localized in a small region of space , " small " being relative to the scale of length of interest to the observer . The proper ...
Page 575
... distribution of radiation , and the total power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M. With the ...
... distribution of radiation , and the total power radiated . 16.3 The uniform charge density of Problem 16.2 is replaced by a uniform density of intrinsic magnetization parallel to the z axis and having total magnetic moment M. With the ...
Page 636
... distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and frequency distribution , general result for accelerated charge , 480 angular distribution of , for ...
... distribution , for magnetic moments , 481 angular and frequency distribution , for ultrarelativistic particle , 481 f . angular and frequency distribution , general result for accelerated charge , 480 angular distribution of , for ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ