Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 82
Page 383
... Consequently for practical purposes he will see only the transverse fields . This equivalence of the fields of a relativistic charged particle and those of a pulse of electromagnetic radiation will be exploited later in Chapter 15 ...
... Consequently for practical purposes he will see only the transverse fields . This equivalence of the fields of a relativistic charged particle and those of a pulse of electromagnetic radiation will be exploited later in Chapter 15 ...
Page 430
John David Jackson. presented . Consequently our discussion will emphasize the physical ideas involved , rather than ... Consequently the momentum impulse Ap is in the transverse direction 430 Classical Electrodynamics Energy transfer in ...
John David Jackson. presented . Consequently our discussion will emphasize the physical ideas involved , rather than ... Consequently the momentum impulse Ap is in the transverse direction 430 Classical Electrodynamics Energy transfer in ...
Page 476
... Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular component alone . In other words , the radiation emitted by a charged particle in arbitrary ...
... Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular component alone . In other words , the radiation emitted by a charged particle in arbitrary ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
18 other sections not shown
Other editions - View all
Common terms and phrases
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