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Page 22
1.8 This expression for energy density is intuitively reasonable, since regions of
high fields “must” contain considerable energy. There is perhaps one puzzling
thing about (1.55). The energy density is positive definite. Consequently its
volume ...
1.8 This expression for energy density is intuitively reasonable, since regions of
high fields “must” contain considerable energy. There is perhaps one puzzling
thing about (1.55). The energy density is positive definite. Consequently its
volume ...
Page 448
The corresponding relativistic expression without the density effect is, from (13.36
), (#) _ (-e)'o. in (o) - | (13.78) dar/b-a co a (00) 2 We see that the density effect
produces a simplification in that the asymptotic energy loss no longer depends
on ...
The corresponding relativistic expression without the density effect is, from (13.36
), (#) _ (-e)'o. in (o) - | (13.78) dar/b-a co a (00) 2 We see that the density effect
produces a simplification in that the asymptotic energy loss no longer depends
on ...
Page 537
(a) Calculate the cross sections for energy transfer Q for close and distant
collisions (write them as functions of Q/I as far as possible and in units of 2mzoe”/
mu°I”). Plot the two distributions for Q|I > 1 for nonrelativistic motion of the incident
...
(a) Calculate the cross sections for energy transfer Q for close and distant
collisions (write them as functions of Q/I as far as possible and in units of 2mzoe”/
mu°I”). Plot the two distributions for Q|I > 1 for nonrelativistic motion of the incident
...
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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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