Classical ElectrodynamicsProblems after each chapter |
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Page 354
... origin ) to detect the arrival time of a light signal from the origin at various points in space . If there is a light source at rest in the system K ( and so moving with velocity v in the negative z direction in system K ' ) which is ...
... origin ) to detect the arrival time of a light signal from the origin at various points in space . If there is a light source at rest in the system K ( and so moving with velocity v in the negative z direction in system K ' ) which is ...
Page 363
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
... origin coincident with that of K at t = 0. An observer in K ' at the point P ' with coordinate x ' is equipped similarly to the one in K. He begins counting when the wave crest passing the origin reaches him , and con- tinues counting ...
Page 436
... origin O. Using the Fourier representations ( 13.16 ) and ( 13.17 ) , as well as that for a delta function ( 2.52 ) ... origin O at an impact parameter b with a velocity v , the electromagnetic fields at the origin are given by ( 11.118 ) ...
... origin O. Using the Fourier representations ( 13.16 ) and ( 13.17 ) , as well as that for a delta function ( 2.52 ) ... origin O at an impact parameter b with a velocity v , the electromagnetic fields at the origin are given by ( 11.118 ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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