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... frame of the particle ( p ' energy of the particle at rest : = 0 ) the scalar product ( 12.5 ) gives the E ' = λ ( 12.6 ) To determine 2 we consider the Lorentz transformation ( 12.4 ) of p , from the rest frame of the particle to the frame ...
... frame of the particle ( p ' energy of the particle at rest : = 0 ) the scalar product ( 12.5 ) gives the E ' = λ ( 12.6 ) To determine 2 we consider the Lorentz transformation ( 12.4 ) of p , from the rest frame of the particle to the frame ...
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... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
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... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . - From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . - From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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