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Page 409
... particle energy by the addition of the potential energy e and by the replacement p → [ P ( e / c ) A ] . These two ... Particle Kinematics and Dynamics Relativistic corrections to the Lagrangian for interacting charged particles,
... particle energy by the addition of the potential energy e and by the replacement p → [ P ( e / c ) A ] . These two ... Particle Kinematics and Dynamics Relativistic corrections to the Lagrangian for interacting charged particles,
Page 443
... particle's trajectory and the typical atom in question if b is comparable to bmax . These atoms , influenced themselves . by the fast particle's fields , will produce perturbing fields at the chosen atom's position , modifying its ...
... particle's trajectory and the typical atom in question if b is comparable to bmax . These atoms , influenced themselves . by the fast particle's fields , will produce perturbing fields at the chosen atom's position , modifying its ...
Page 520
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
... particle " and a " struck system . " The perturbing fields of the incident particle are replaced by an equivalent pulse of radiation which is analyzed into a frequency spectrum of virtual quanta . Then the effects of the quanta ( either ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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Common terms and phrases
4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ