Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 76
Page 406
... motion as d ( ymv ) = 0 dt ( 12.67 ) - where y = [ 1 ( v2 / c2 ) ] . At the least sophisticated level we know that the Lagrangian L must be chosen strategically so that the Euler - Lagrange equations of motion , - daL ƏL dt aqi да = 0 ...
... motion as d ( ymv ) = 0 dt ( 12.67 ) - where y = [ 1 ( v2 / c2 ) ] . At the least sophisticated level we know that the Lagrangian L must be chosen strategically so that the Euler - Lagrange equations of motion , - daL ƏL dt aqi да = 0 ...
Page 578
... motions of charged particles or currents are calculated . Antennas and radiation from multipole sources are examples of the first type of problem , while motion of charges in electric and magnetic fields and energy - loss phenomena are ...
... motions of charged particles or currents are calculated . Antennas and radiation from multipole sources are examples of the first type of problem , while motion of charges in electric and magnetic fields and energy - loss phenomena are ...
Page 581
... motion will be unimportant . The examples of the last two paragraphs show that the reactive effects of radiation on the motion of a charged particle can be expected to be important if the external forces are such that the motion changes ...
... motion will be unimportant . The examples of the last two paragraphs show that the reactive effects of radiation on the motion of a charged particle can be expected to be important if the external forces are such that the motion changes ...
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