Chapter 12: Q12.38P (page 549)
Show that it is possible to outrun a light ray, if you're given a sufficient head start, and your feet generate a constant force.
Short Answer
It is possible to outrun a light ray.
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Chapter 12: Q12.38P (page 549)
Show that it is possible to outrun a light ray, if you're given a sufficient head start, and your feet generate a constant force.
It is possible to outrun a light ray.
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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.
An ideal magnetic dipole moment m is located at the origin of an inertial system that moves with speed v in the x direction with respect to inertial system S. In the vector potential is
(Eq. 5.85), and the scalar potential is zero.
(a) Find the scalar potential V in S.
(b) In the nonrelativistic limit, show that the scalar potential in S is that of an ideal electric dipole of magnitude
located at .

Consider a particle in hyperbolic motion,
(a) Find the proper time role="math" localid="1654682576730" as a function of , assuming the clocks are set so that when . [Hint: Integrate Eq. 12.37.]
(b) Find x and v (ordinary velocity) as functions of .
(c) Find (proper velocity) as a function of .
“In 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?
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).
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