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Page 392
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
... particles behave kinematically in the same way , whether charged or neutral . A charged particle can be thought of as a very localized distribution of charge and mass . To find the force acting on such a particle we integrate the ...
Page 393
... particle ( p ' = 0 ) the scalar product ( 12.5 ) gives the energy of the particle at rest : E ' = λ ( 12.6 ) To determine & we consider the Lorentz transformation ( 12.4 ) of Ри from the rest frame of the particle to the frame K in ...
... particle ( p ' = 0 ) the scalar product ( 12.5 ) gives the energy of the particle at rest : E ' = λ ( 12.6 ) To determine & we consider the Lorentz transformation ( 12.4 ) of Ри from the rest frame of the particle to the frame K in ...
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,
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ