Classical ElectrodynamicsProblems after each chapter |
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Page 16
... problem . This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is plausible that specification of the electric field ( normal derivative of the potential ) every- where on the surface ( corresponding to a ...
... problem . This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is plausible that specification of the electric field ( normal derivative of the potential ) every- where on the surface ( corresponding to a ...
Page 27
... problem is on the left , the equivalent - image problem on the right . -q are called image charges , and the replacement of the actual problem with boundaries by an enlarged region with image charges but no boundaries is called the ...
... problem is on the left , the equivalent - image problem on the right . -q are called image charges , and the replacement of the actual problem with boundaries by an enlarged region with image charges but no boundaries is called the ...
Page 186
... problem is an initial - value problem with y ( x , tô ) and dy ( x , tô ) / dt given for all x . We wish to determine y ( x , t ) for all times t > to . To discuss the initial - value problem and also an integral representation of ...
... problem is an initial - value problem with y ( x , tô ) and dy ( x , tô ) / dt given for all x . We wish to determine y ( x , t ) for all times t > to . To discuss the initial - value problem and also an integral representation of ...
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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