Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 49
Page 472
... acceleration . For relativistic motion behavior the acceleration fields depend on the velocity as well as the acceleration . Consequently the angular distribution is more complicated . From ( 14.14 ) the radial component of Poynting's ...
... acceleration . For relativistic motion behavior the acceleration fields depend on the velocity as well as the acceleration . Consequently the angular distribution is more complicated . From ( 14.14 ) the radial component of Poynting's ...
Page 475
... acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion ... acceleration is a factor of y2 larger than with a parallel acceleration . 14.4 Radiation Emitted by a Charge in ...
... acceleration perpendicular to the velocity ( 14.46 ) for the same magnitude of applied force . For circular motion ... acceleration is a factor of y2 larger than with a parallel acceleration . 14.4 Radiation Emitted by a Charge in ...
Page 506
... acceleration and emits radiation . If its collision partner is also a charged particle , they both emit radiation and a coherent superposition of the radiation fields must be made . Since the amplitude of the radiation fields depends ...
... acceleration and emits radiation . If its collision partner is also a charged particle , they both emit radiation and a coherent superposition of the radiation fields must be made . Since the amplitude of the radiation fields depends ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
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