Classical ElectrodynamicsProblems after each chapter |
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Page 52
... radius a is in a uniform electric field E. If the sphere is cut into two hemispheres by a plane perpendicular to the field , find the force required to prevent the hemispheres from separa- ting ( a ) if the shell is uncharged ; ( b ) if ...
... radius a is in a uniform electric field E. If the sphere is cut into two hemispheres by a plane perpendicular to the field , find the force required to prevent the hemispheres from separa- ting ( a ) if the shell is uncharged ; ( b ) if ...
Page 307
... radius a and outer radius b has its axis along the negative z axis . Both inner and outer conductors end at z = O , and the outer one is connected to an infinite plane flange occupy- ing the whole x - y plane ( except for the annulus of ...
... radius a and outer radius b has its axis along the negative z axis . Both inner and outer conductors end at z = O , and the outer one is connected to an infinite plane flange occupy- ing the whole x - y plane ( except for the annulus of ...
Page 576
... radius a in a conducting medium can serve as an electromagnetic resonant cavity . 16.9 ( a ) Assuming infinite conductivity , determine the transcendental equations for the characteristic frequencies win of the cavity for TE and TM ...
... radius a in a conducting medium can serve as an electromagnetic resonant cavity . 16.9 ( a ) Assuming infinite conductivity , determine the transcendental equations for the characteristic frequencies win of the cavity for TE and TM ...
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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