Classical Electrodynamics |
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Page 51
2 A point charge q is brought to a position a distance d away from an infinite
plane conductor held at zero potential . Using the method of images , find : ( a )
the surface - charge density induced on the plane , and plot it ; ( b ) the force
between ...
2 A point charge q is brought to a position a distance d away from an infinite
plane conductor held at zero potential . Using the method of images , find : ( a )
the surface - charge density induced on the plane , and plot it ; ( b ) the force
between ...
Page 220
E PARALLEL TO PLANE OF INCIDENCE E• ' = 2 / Hesin 21 2 cos i sin sin ( i + r )
cos ( i - p ) sin 2r + sin 2i u ' ( 7 . 60 ) - , sin 2i – sin 2r tan ( i – r ) tan ( i + r ) O sin 2r
+ ļ sin 2 ; Again the results on the right apply for ui ' = M . For normal incidence ...
E PARALLEL TO PLANE OF INCIDENCE E• ' = 2 / Hesin 21 2 cos i sin sin ( i + r )
cos ( i - p ) sin 2r + sin 2i u ' ( 7 . 60 ) - , sin 2i – sin 2r tan ( i – r ) tan ( i + r ) O sin 2r
+ ļ sin 2 ; Again the results on the right apply for ui ' = M . For normal incidence ...
Page 307
A linearly polarized plane wave of amplitude E , and wave number k is incident
on a circular opening of radius a in an otherwise perfectly conducting flat screen .
The incident wave vector makes an angle « with the normal to the screen .
A linearly polarized plane wave of amplitude E , and wave number k is incident
on a circular opening of radius a in an otherwise perfectly conducting flat screen .
The incident wave vector makes an angle « with the normal to the screen .
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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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