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 198
... discussed in almost all textbooks . A good treatment of the energy of quasi - stationary currents and forces acting ... discussed with many examples by Smythe , Chapter XI . The mathematical topics in this chapter center around the wave ...
... discussed in almost all textbooks . A good treatment of the energy of quasi - stationary currents and forces acting ... discussed with many examples by Smythe , Chapter XI . The mathematical topics in this chapter center around the wave ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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