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Page 393
... particle ( p ' = 0 ) the scalar product ( 12.5 ) gives the energy of the particle at rest : E ' = λ ( 12.6 ) To determine λ we consider the Lorentz transformation ( 12.4 ) of p1 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 λ we consider the Lorentz transformation ( 12.4 ) of p1 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,
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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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ