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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 ve = ( 7.32 ) dk lo If an energy density is associated with the magnitude of the wave ...
This shows that , apart from an overall phase factor , the pulse travels along undistorted in shape with a velocity , called the group velocity : do ve = ( 7.32 ) dk lo If an energy density is associated with the magnitude of the wave ...
Page 331
where we have introduced a vectorial Alfvén velocity : B. ( 10.70 ) Va = V4πρ I - iwt The wave equation ( 10.69 ) for vi is somewhat involved , but it allows simple solutions for waves propagating parallel or perpendicular to the ...
where we have introduced a vectorial Alfvén velocity : B. ( 10.70 ) Va = V4πρ I - iwt The wave equation ( 10.69 ) for vi is somewhat involved , but it allows simple solutions for waves propagating parallel or perpendicular to the ...
Page 340
For wave numbers k < kd , the phase and group velocities of the longitudinal plasma oscillations are : 31 k ( 10.107 ) 3 ( u ) Vo = Up From the definition of ko we see that for such wave numbers the phase velocity is much larger than ...
For wave numbers k < kd , the phase and group velocities of the longitudinal plasma oscillations are : 31 k ( 10.107 ) 3 ( u ) Vo = Up From the definition of ko we see that for such wave numbers the phase velocity is much larger than ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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