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 : ( 7 . 32 ) If an
energy density is associated with the magnitude of the wave ( or its absolute
square ) , it ...
This shows that , apart from an overall phase factor , the pulse travels along
undistorted in shape with a velocity , called the group velocity : ( 7 . 32 ) If an
energy density is associated with the magnitude of the wave ( or its absolute
square ) , it ...
Page 331
where we have introduced a vectorial Alfvén velocity : ( 10 . 70 ) The wave
equation ( 10 . 69 ) for v , is somewhat involved , but it allows simple solutions for
waves propagating parallel or perpendicular to the magnetic field direction . *
With vz ...
where we have introduced a vectorial Alfvén velocity : ( 10 . 70 ) The wave
equation ( 10 . 69 ) for v , is somewhat involved , but it allows simple solutions for
waves propagating parallel or perpendicular to the magnetic field direction . *
With vz ...
Page 340
107 ) From the definition of kp 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 ( u2 ) . As the wave number increases towards kp , the phase
velocity ...
107 ) From the definition of kp 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 ( u2 ) . As the wave number increases towards kp , the phase
velocity ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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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 modes 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 |