Classical Electrodynamics |
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Page 213
This means that at times immediately before t = 0 the wave consisted of _ two
pulses , both moving towards the origin , such that at t = 0 they coalesced into the
shape given by ( 7 . 38 ) . Clearly at later times we expect each pulse to re ...
This means that at times immediately before t = 0 the wave consisted of _ two
pulses , both moving towards the origin , such that at t = 0 they coalesced into the
shape given by ( 7 . 38 ) . Clearly at later times we expect each pulse to re ...
Page 363
If the wave crest passing the origin at t = 0 is the first one which he records ( when
it reaches him ) , then at time t he will have counted - ( k · X – wt ) wave crests .
Now imagine another reference frame K ' which moves relative to the frame K ...
If the wave crest passing the origin at t = 0 is the first one which he records ( when
it reaches him ) , then at time t he will have counted - ( k · X – wt ) wave crests .
Now imagine another reference frame K ' which moves relative to the frame K ...
Page 370
The unshaded interior of the cone represents the past and the future , while the
shaded region outside the cone is called “ elsewhere . ” A point inside ( outside )
the light cone is said to have a time - like ( spacelike ) separation from the origin .
The unshaded interior of the cone represents the past and the future , while the
shaded region outside the cone is called “ elsewhere . ” A point inside ( outside )
the light cone is said to have a time - like ( spacelike ) separation from the origin .
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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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