Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 80
Page 514
... relativistic bremsstrahlung calculation can be done nonrelativistically . There are two aspects . First of all , we know that radiation emitted by a highly relativistic particle is confined to a narrow cone of half - angle of the order ...
... relativistic bremsstrahlung calculation can be done nonrelativistically . There are two aspects . First of all , we know that radiation emitted by a highly relativistic particle is confined to a narrow cone of half - angle of the order ...
Page 632
... relativistic , 394 f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188 use of , in diffraction , 280 vector equivalent of , 283 Klein - Nishina formula , 490 Lagrangian , for relativistic charge par ...
... relativistic , 394 f . Kirchhoff diffraction , see Diffraction Kirchhoff's integral representation , 188 use of , in diffraction , 280 vector equivalent of , 283 Klein - Nishina formula , 490 Lagrangian , for relativistic charge par ...
Page 637
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
... Relativistic notation , 377 Relativistic transformation , and Thomas precession , 367 from CM system to laboratory , 400 f . of acceleration , 388 of charge and current densities , 378 of coordinates , 357 of electromagnetic fields ...
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