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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 : 22 ཀྵུ ། " ( 12.5 ) 0 ) the scalar product ( 12.5 ) gives the ( p⋅ p ) = ( p ' · p ' ) = In the rest frame of the particle ( p ' energy of the particle at rest : = E ' = λ ( 12.6 ) To determine & we consider the Lorentz ...
... particle : 22 ཀྵུ ། " ( 12.5 ) 0 ) the scalar product ( 12.5 ) gives the ( p⋅ p ) = ( p ' · p ' ) = In the rest frame of the particle ( p ' energy of the particle at rest : = E ' = λ ( 12.6 ) To determine & we consider the Lorentz ...
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 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ