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Page 397
... involved and to see the processes in their simplest form kinematically it is convenient to transform to a coordinate frame K ' , where the projectile and the target have equal and oppositely directed momenta . This frame is called the ...
... involved and to see the processes in their simplest form kinematically it is convenient to transform to a coordinate frame K ' , where the projectile and the target have equal and oppositely directed momenta . This frame is called the ...
Page 506
... involved produces quantum - mechanical modifications very similar to those appearing in our earlier energy - loss considerations . These can be taken into account in a relatively simple way . But there is a more serious deficiency which ...
... involved produces quantum - mechanical modifications very similar to those appearing in our earlier energy - loss considerations . These can be taken into account in a relatively simple way . But there is a more serious deficiency which ...
Page 599
... involved . The acausal effects are limited to time intervals of the order of 7 ~ e2 / mc3 ~ 10 -24 sec . This is the time it takes light to travel a distance of the order of the " size " of elementary particles . Such a short time ...
... involved . The acausal effects are limited to time intervals of the order of 7 ~ e2 / mc3 ~ 10 -24 sec . This is the time it takes light to travel a distance of the order of the " size " of elementary particles . Such a short time ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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 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