Classical ElectrodynamicsProblems after each chapter |
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Page 117
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
... seen as follows . Suppose that inside the sphere we have a cubic array of dipoles such as are shown in Fig . 4.12 , with all their moments constant in magnitude and oriented along the same direction ( remember that the sphere is ...
Page 155
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield · ( B2- B1 ) n = 0 ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in ...
... shown in Fig . 5.9 , Gauss's theorem can be applied to V. B = 0 to yield · ( B2- B1 ) n = 0 ( 5.88 ) where n is the unit normal to the surface directed from region 1 into region 2 , and the subscripts refer to values at the surface in ...
Page 327
... described . The first is the kink instability , shown in Fig . 10.8a . The lines of azimu- thal magnetic induction near the column are bunched together above , and separated below , the column by the distortion downwards . Thus the ...
... described . The first is the kink instability , shown in Fig . 10.8a . The lines of azimu- thal magnetic induction near the column are bunched together above , and separated below , the column by the distortion downwards . Thus the ...
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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