Classical ElectrodynamicsProblems after each chapter |
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Page 286
... side of Fig . 9.5 . We do not care about the values of the fields in region II ' . In fact , the hypothetical sources inside the disc will be imagined to be such that the fields in region II ' give a contribution to the surface integral ...
... side of Fig . 9.5 . We do not care about the values of the fields in region II ' . In fact , the hypothetical sources inside the disc will be imagined to be such that the fields in region II ' give a contribution to the surface integral ...
Page 392
... sides with respect to time , then the left - hand side becomes the momentum or energy of the particle while the right - hand side is the four - dimensional integral of f . Since d'r is a Lorentz invariant quantity , it follows that p1 ...
... sides with respect to time , then the left - hand side becomes the momentum or energy of the particle while the right - hand side is the four - dimensional integral of f . Since d'r is a Lorentz invariant quantity , it follows that p1 ...
Page 567
... sides of ( 16.22 ) . Then we can put | x ' | - | x − x ' | ~ r ' — nx on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r = r . Furthermore we can - - = r ' and r < use the asymptotic form ...
... sides of ( 16.22 ) . Then we can put | x ' | - | x − x ' | ~ r ' — nx on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r = r . Furthermore we can - - = r ' and r < use the asymptotic form ...
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