Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 64
Page
... particle ( p ' energy of the particle at rest : = 0 ) the scalar product ( 12.5 ) gives the E ' = λ ( 12.6 ) To determine 2 we consider the Lorentz transformation ( 12.4 ) of p , from the rest frame of the particle to the frame K in ...
... particle ( p ' energy of the particle at rest : = 0 ) the scalar product ( 12.5 ) gives the E ' = λ ( 12.6 ) To determine 2 we consider the Lorentz transformation ( 12.4 ) of p , from the rest frame of the particle to the frame K in ...
Page
... particle is initially at rest . From definition ( 11.62 ) of proper time it is clear that , if the particle stays at rest in that frame , the integral over proper time will be larger than if it moves with a nonzero velocity along its ...
... particle is initially at rest . From definition ( 11.62 ) of proper time it is clear that , if the particle stays at rest in that frame , the integral over proper time will be larger than if it moves with a nonzero velocity along its ...
Page
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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