Classical ElectrodynamicsProblems after each chapter |
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Page 104
... average over them at that instant will yield the same result as an average at some later instant of time . Hence , as far as the averaged quantities are concerned , it is legitimate to talk of static fields and charges . * Furthermore ...
... average over them at that instant will yield the same result as an average at some later instant of time . Hence , as far as the averaged quantities are concerned , it is legitimate to talk of static fields and charges . * Furthermore ...
Page 321
... average pressure , total current , and radius of the cylinder of fluid or plasma confined by its own magnetic field . Note that the average pressure of the matter is equal to the magnetic pressure ( B2 / 8 ) at the surface of the ...
... average pressure , total current , and radius of the cylinder of fluid or plasma confined by its own magnetic field . Note that the average pressure of the matter is equal to the magnetic pressure ( B2 / 8 ) at the surface of the ...
Page 416
... average value , VG = ( V1 ) = ( 1B ) w дв wo x ( ( xo ) , ( n⋅ xo ) ) ( 12.107 ) To determine the average value of ( x ) ( n⋅ x ) , it is necessary only to observe that the rectangular components of ( x ) , oscillate sinusoidally with ...
... average value , VG = ( V1 ) = ( 1B ) w дв wo x ( ( xo ) , ( n⋅ xo ) ) ( 12.107 ) To determine the average value of ( x ) ( n⋅ x ) , it is necessary only to observe that the rectangular components of ( x ) , oscillate sinusoidally with ...
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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