Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 76
Page 210
... wave number . The pulse shown at t = 0 in Fig . 7.5 begins to move as time goes on . The different frequency or wave - number components in it move at different phase velocities . Consequently there is a tendency for the original ...
... wave number . The pulse shown at t = 0 in Fig . 7.5 begins to move as time goes on . The different frequency or wave - number components in it move at different phase velocities . Consequently there is a tendency for the original ...
Page 245
... wave number k is determined for each value of λ : @ 2 k12 = με - γλ c2 If we define a cutoff frequency w ወ = [ c ] με then the wave number can be written : kλ = 2 ― ( 8.37 ) ( 8.38 ) * ( 8.39 ) * We note that , for w > w , the wave ...
... wave number k is determined for each value of λ : @ 2 k12 = με - γλ c2 If we define a cutoff frequency w ወ = [ c ] με then the wave number can be written : kλ = 2 ― ( 8.37 ) ( 8.38 ) * ( 8.39 ) * We note that , for w > w , the wave ...
Page 333
... wave number ) , but decreases with increasing magnetic field strength . In terms of the diffusion time of Section 10.3 , the imaginary part of the wave number shows that , apart from viscosity effects , the wave travels for a time ...
... wave number ) , but decreases with increasing magnetic field strength . In terms of the diffusion time of Section 10.3 , the imaginary part of the wave number shows that , apart from viscosity effects , the wave travels for a time ...
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