Classical Electrodynamics |
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Page 392
For neutral particles with no detectable electromagnetic interactions it is clearly
impossible to obtain their relativistic transformation properties in this ... A charged
particle can be thought of as a very localized distribution of charge and mass.
For neutral particles with no detectable electromagnetic interactions it is clearly
impossible to obtain their relativistic transformation properties in this ... A charged
particle can be thought of as a very localized distribution of charge and mass.
Page 393
The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic
of the particle: 2. (pop). = (p. 2)--. (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' = A (12.6) To ...
The length of the 4-vector p, is a Lorentz invariant quantity which is characteristic
of the particle: 2. (pop). = (p. 2)--. (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' = A (12.6) To ...
Page 417
12.7 (a) Particle moving in helical path along lines of uniform, constant magnetic
induction. (b) Curvature of lines of magnetic induction will cause drift
perpendicular to the (r, y) plane. |VB|B|< 1, the drift velocity is small compared to
the orbital ...
12.7 (a) Particle moving in helical path along lines of uniform, constant magnetic
induction. (b) Curvature of lines of magnetic induction will cause drift
perpendicular to the (r, y) plane. |VB|B|< 1, the drift velocity is small compared to
the orbital ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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