Classical ElectrodynamicsProblems after each chapter |
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Page 297
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
Page 324
... compared to the radius , the dynamic behavior is characteristic of hydrodynamic shock waves . But for a hot , tenuous plasma the mean free path is comparable to , or larger than , the radius . Then a model with particles moving freely ...
... compared to the radius , the dynamic behavior is characteristic of hydrodynamic shock waves . But for a hot , tenuous plasma the mean free path is comparable to , or larger than , the radius . Then a model with particles moving freely ...
Page 432
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to 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