Classical Electrodynamics |
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Page 297
Then both scalar and vector approximations reduce to the common expression,
dP (ka)*|J1(ka sin 6) = ~ P, So- |+}d() T ka sin 6 The vector and scalar Kirchhoff
approximations are compared in Fig. 9.11 for the angle of incidence equal to 45°
...
Then both scalar and vector approximations reduce to the common expression,
dP (ka)*|J1(ka sin 6) = ~ P, So- |+}d() T ka sin 6 The vector and scalar Kirchhoff
approximations are compared in Fig. 9.11 for the angle of incidence equal to 45°
...
Page 324
If the mean free path for collisions is short compared to the radius, the dynamic
behavior is characteristic of hydrodynamic shock waves. But for a hot, tenuous
plasma the mean free path is comparable to, or larger than, the radius. Then a ...
If the mean free path for collisions is short compared to the radius, the dynamic
behavior is characteristic of hydrodynamic shock waves. But for a hot, tenuous
plasma the mean free path is comparable to, or larger than, the radius. Then a ...
Page 432
As long as the distance d it actually moves is small compared to b, we may
expect that (13.2) will be correct. An estimate of d can be obtained by saying that
Ap/2m is an average velocity of the electron during the collision, and that the time
of ...
As long as the distance d it actually moves is small compared to b, we may
expect that (13.2) will be correct. An estimate of d can be obtained by saying that
Ap/2m is an average velocity of the electron during the collision, and that the time
of ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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