Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 70
Page 211
... velocity , called the group velocity : Vg = dw dk lo ( 7.32 ) If an energy density is associated with the magnitude of the wave ( or its absolute square ) , it is clear that in this approximation the transport of energy occurs with the ...
... velocity , called the group velocity : Vg = dw dk lo ( 7.32 ) If an energy density is associated with the magnitude of the wave ( or its absolute square ) , it is clear that in this approximation the transport of energy occurs with the ...
Page 331
... velocity equal to the sound velocity s . But there is also a transverse wave ( V1 0 ) with a phase velocity equal to the Alfvén velocity v . This Alfvén wave is a purely magnetohydrodynamic phenomenon which depends only on the magnetic ...
... velocity equal to the sound velocity s . But there is also a transverse wave ( V1 0 ) with a phase velocity equal to the Alfvén velocity v . This Alfvén wave is a purely magnetohydrodynamic phenomenon which depends only on the magnetic ...
Page 367
... velocity v + dv . The increment in velocity is related to the electron's acceleration a by dv = a dt . At time t the electron's rest frame K ' and the laboratory frame K are related by a Lorentz transformation with velocity v . At time ...
... velocity v + dv . The increment in velocity is related to the electron's acceleration a by dv = a dt . At time t the electron's rest frame K ' and the laboratory frame K are related by a Lorentz transformation with velocity v . At 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