Chapter 12: Q54P (page 568)
Show that the second equation in Eq. 12.127 can be expressed in terms of the field tensor as follows:
localid="1654746948628"
Short Answer
The second equation can be expressed in terms of field tensor as
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Chapter 12: Q54P (page 568)
Show that the second equation in Eq. 12.127 can be expressed in terms of the field tensor as follows:
localid="1654746948628"
The second equation can be expressed in terms of field tensor as
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Inertial system S moves at constant velocity with respect to S. Their axes are parallel to one other, and their origins coincide at data-custom-editor="chemistry" , as usual. Find the Lorentz transformation matrix A.
Prove that the symmetry (or antisymmetry) of a tensor is preserved by Lorentz transformation (that is: if is symmetric, show that is also symmetric, and likewise for antisymmetric).
鈥淚n a certain inertial frame S, the electric field E and the magnetic field B are neither parallel nor perpendicular, at a particular space-time point. Show that in a different inertial system , moving relative to S with velocity v given by
the fieldsare parallel at that point. Is there a frame in which the two are perpendicular?
A particle of mass m collides elastically with an identical particle at rest. Classically, the outgoing trajectories always make an angle of . Calculate this angle relativistically, in terms of , the scattering angle, and v, the speed, in the center-of-momentum frame.
The natural relativistic generalization of the Abraham-Lorentz formula (Eq. 11.80) would seem to be
This is certainly a 4-vector, and it reduces to the Abraham-Lorentz formula in the non-relativistic limit .
(a) Show, nevertheless, that this is not a possible Minkowski force.
(b) Find a correction term that, when added to the right side, removes the objection you raised in (a), without affecting the 4-vector character of the formula or its non-relativistic limit.
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