Classical ElectrodynamicsProblems after each chapter |
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Page ix
... discussed in Chapter 11 , where all the necessary formal apparatus is developed , various kinematic consequences are explored , and the covariance of electrodynamics is established . The next chapter is devoted to relativistic particle ...
... discussed in Chapter 11 , where all the necessary formal apparatus is developed , various kinematic consequences are explored , and the covariance of electrodynamics is established . The next chapter is devoted to relativistic particle ...
Page 93
... discussed the charged conducting disc in cylindrical coordinates in order to illustrate the complications of mixed boundary conditions . For this particular example , the mixed boundary conditions can be avoided by separating Laplace's ...
... discussed the charged conducting disc in cylindrical coordinates in order to illustrate the complications of mixed boundary conditions . For this particular example , the mixed boundary conditions can be avoided by separating Laplace's ...
Page 268
... discussed the properties of electro- magnetic waves and their propagation in both bounded and unbounded geometries ... discussed . The second half of the chapter is devoted to the subject of diffraction . Since the customary scalar ...
... discussed the properties of electro- magnetic waves and their propagation in both bounded and unbounded geometries ... discussed . The second half of the chapter is devoted to the subject of diffraction . Since the customary scalar ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ