Classical Electrodynamics |
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Page 354
For convenience we suppose that a common origin of time t = t = 0 is chosen at
the instant when the two sets of coordinate ... at known distances from the origin)
to detect the arrival time of a light signal from the origin at various points in space.
For convenience we suppose that a common origin of time t = t = 0 is chosen at
the instant when the two sets of coordinate ... at known distances from the origin)
to detect the arrival time of a light signal from the origin at various points in space.
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 1 k • x — ot 3." ot) 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 1 k • x — ot 3." ot) wave crests.
Now imagine another reference frame K' which moves relative to the frame K ...
Page 436
Consequently AE = es v - E dt (13.22) where v = x, and in the dipole
approximation E is the field of the incident particle at the origin O. Using the
Fourier representations (13.16) and (13.17), as well as that for a delta function (
2.52), and the ...
Consequently AE = es v - E dt (13.22) where v = x, and in the dipole
approximation E is the field of the incident particle at the origin O. Using the
Fourier representations (13.16) and (13.17), as well as that for a delta function (
2.52), and the ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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