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 acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ