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For a charged particle the force is the Lorentz force . Since we have discussed
the Lorentz transformation properties of the Lorentz force density in Section 11 .
11 , we can immediately deduce the behavior of a charged particle ' s momentum
The length of the 4 - vector p is a Lorentz invariant quantity which is characteristic
of the particle : ( 12 . 5 ) ( p • p ) = ( p ? . p " ) = - In the rest frame of the particle ( p '
= 0 ) the scalar product ( 12 . 5 ) gives the energy of the particle at rest : E ' = 2 ...
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 into ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
RelativisticParticle Kinematics and Dynamics
8 other sections not shown