Classical Electrodynamics |
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Page 211
This shows that, apart from an overall phase factor, the pulse travels along
undistorted in shape with a velocity, called the group velocity: do * = I. o (7.32) If
an energy density is associated with the magnitude of the wave (or its absolute
square) ...
This shows that, apart from an overall phase factor, the pulse travels along
undistorted in shape with a velocity, called the group velocity: do * = I. o (7.32) If
an energy density is associated with the magnitude of the wave (or its absolute
square) ...
Page 340
T. 10.107 3(u”) ( ) 1) *-w 1) w p From the definition of ko we see that for such
wave numbers the phase velocity is much larger than, and the group velocity
much smaller than, the rms thermal velocity (u”)*. As the wave number increases
...
T. 10.107 3(u”) ( ) 1) *-w 1) w p From the definition of ko we see that for such
wave numbers the phase velocity is much larger than, and the group velocity
much smaller than, the rms thermal velocity (u”)*. As the wave number increases
...
Page 494
But a particle moving with constant velocity through a material medium can
radiate if its velocity is greater than the phase velocity of light in the medium.
Such radiation is called Cherenkov radiation, after its discoverer, P. A. Cherenkov
(1937).
But a particle moving with constant velocity through a material medium can
radiate if its velocity is greater than the phase velocity of light in the medium.
Such radiation is called Cherenkov radiation, after its discoverer, P. A. Cherenkov
(1937).
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
5 other sections not shown
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |