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 . 1 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 . 1 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 91
... problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first solved the present problem by using certain discontinuous integrals involving Bessel functions . Titchmarsh , p . 334 , uses ...
... problem and variations of it have received considerable attention over the years . H. Weber ( 1873 ) first solved the present problem by using certain discontinuous integrals involving Bessel functions . Titchmarsh , p . 334 , uses ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ