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At time t the electron's rest frame K' and the laboratory frame K are related by a
Lorentz transformation with velocity v. At time t + 6t the electron's rest frame has
now changed to K", related to K by a Lorentz transformation with velocity v + 6v.
This is then exactly the requirement that Lorentz transformations are rotations in a
four-dimensional Euclidean space or, ... The Lorentz transformation (11.21) can
be written in the general form: ' — ar, - aaya, u = 1, 2, 3, 4 (11.70) v 3. where the ...
0 (11.112) 11.10 Transformation of the Electromagnetic Fields Since the fields E
and B are elements of the field-strength tensor F., their transformation properties
can be found from Fiv = a,zav, Fa, (11.113) With transformation (11.75) from a ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
BoundaryValue Problems in Electrostatics II
16 other sections not shown