Classical Electrodynamics |
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Page 39
The potential has the constant value Q / R inside the sphere and falls off inversely
with distance away from the center for points outside the sphere . By a suitable
choice of center of inversion and associated parameters we can obtain the ...
The potential has the constant value Q / R inside the sphere and falls off inversely
with distance away from the center for points outside the sphere . By a suitable
choice of center of inversion and associated parameters we can obtain the ...
Page 96
( b ) Show that the potential a perpendicular distance z above the center of the
disc is 0 , 0 ) = v ( 1 - vata ) ( c ) Show that the potential a perpendicular distance z
above the edge of the disc is Po ( 2 ) = [ E ( k ) – ( 1 – k ) K ( K ) ] where k = 2a / (
22 ...
( b ) Show that the potential a perpendicular distance z above the center of the
disc is 0 , 0 ) = v ( 1 - vata ) ( c ) Show that the potential a perpendicular distance z
above the edge of the disc is Po ( 2 ) = [ E ( k ) – ( 1 – k ) K ( K ) ] where k = 2a / (
22 ...
Page 225
The field energy is almost entirely magnetic in nature . The waves given by ( 7 .
80 ) show an exponential damping with distance . This means that an
electromagnetic wave entering a conductor is damped to 1 / e = 0 . 369 of its
initial amplitude ...
The field energy is almost entirely magnetic in nature . The waves given by ( 7 .
80 ) show an exponential damping with distance . This means that an
electromagnetic wave entering a conductor is damped to 1 / e = 0 . 369 of its
initial amplitude ...
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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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