Classical Electrodynamics |
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The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic
of the particle: 2 (p → p) = (p'' p') = — : (12.5) In the rest frame of the particle (p = 0
) the scalar product (12.5) gives the energy of the particle at rest: - E' = 2 (12.6) ...
The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic
of the particle: 2 (p → p) = (p'' p') = — : (12.5) In the rest frame of the particle (p = 0
) the scalar product (12.5) gives the energy of the particle at rest: - E' = 2 (12.6) ...
Page
Since (p → p) = —m”, we see that for a free particle y L, is a constant, yL, - – A (
12.72) Then the action is proportional to the integral of the proper time over the
path from the initial space-time point a to the final space-time point b. This
integral is ...
Since (p → p) = —m”, we see that for a free particle y L, is a constant, yL, - – A (
12.72) Then the action is proportional to the integral of the proper time over the
path from the initial space-time point a to the final space-time point b. This
integral is ...
Page
15.5 Weizsäcker-Williams Method of Virtual Quanta The emission of
bremsstrahlung and other processes involving the electromagnetic interaction of
relativistic particles can be viewed in a way that is very helpful in providing
physical insight ...
15.5 Weizsäcker-Williams Method of Virtual Quanta The emission of
bremsstrahlung and other processes involving the electromagnetic interaction of
relativistic particles can be viewed in a way that is very helpful in providing
physical insight ...
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Contents
Introduction to Electrostatics | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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