Classical Electrodynamics |
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Page 96
2 , using the appropriate Green ' s function obtained in the text , and verify that the
answer obtained in this way agrees ... 12 ( a ) Verify that - 8lp - p ) = 1 kJm ( kp ) J
mlkp ' ) dk ( 6 ) Obtain the following expansion : m ( bRoxy = 2 dk eim ( 6 – ' !
2 , using the appropriate Green ' s function obtained in the text , and verify that the
answer obtained in this way agrees ... 12 ( a ) Verify that - 8lp - p ) = 1 kJm ( kp ) J
mlkp ' ) dk ( 6 ) Obtain the following expansion : m ( bRoxy = 2 dk eim ( 6 – ' !
Page 403
4 Laboratory angle 0 , of particle 3 versus center of momentum angle for a < 1
and a > 1 . it is a straightforward , although tedious , matter to obtain the result : (
E + məsme + m ; * + mı ? 7 m ; ? – mi ? ) lup cos 0 , [ ( m2€ + m ; + m , mo ? – m ; )
...
4 Laboratory angle 0 , of particle 3 versus center of momentum angle for a < 1
and a > 1 . it is a straightforward , although tedious , matter to obtain the result : (
E + məsme + m ; * + mı ? 7 m ; ? – mi ? ) lup cos 0 , [ ( m2€ + m ; + m , mo ? – m ; )
...
Page 498
Then we obtain dI ( W ) e 12 I 2TT J - ( 14 . 127 ) dS2 C3 The integral is a Dirac
delta ... To obtain a meaningful result we assume that the particle passes through
a slab of dielectric in a time interval 27 . Then the infinite integral in ( 14 . 127 ) is
...
Then we obtain dI ( W ) e 12 I 2TT J - ( 14 . 127 ) dS2 C3 The integral is a Dirac
delta ... To obtain a meaningful result we assume that the particle passes through
a slab of dielectric in a time interval 27 . Then the infinite integral in ( 14 . 127 ) is
...
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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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