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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 çoalesced 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 çoalesced 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 = O is the first one which he records ( when it reaches him ) , then at time t he will have counted ( k · X2п wt ) wave crests . Now imagine another reference frame K ' which moves relative to ...
If the wave crest passing the origin at t = O is the first one which he records ( when it reaches him ) , then at time t he will have counted ( k · X2п wt ) wave crests . Now imagine another reference frame K ' which moves relative to ...
Page 370
A point inside ( outside ) the light cone is said to have a time - like ( spacelike ) separation from the origin . Past T2 = derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will ...
A point inside ( outside ) the light cone is said to have a time - like ( spacelike ) separation from the origin . Past T2 = derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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