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Page 208
... considers making a linear superposition . Initially we will find it most convenient to use k as an independent variable . To allow for the possibility of dispersion we will consider w as a general function of k : @ = w ( k ) ( 7.25 ) ...
... considers making a linear superposition . Initially we will find it most convenient to use k as an independent variable . To allow for the possibility of dispersion we will consider w as a general function of k : @ = w ( k ) ( 7.25 ) ...
Page 358
... Consider a rod of length Lo at rest parallel to the z ' axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition L1 = z2- z ' , where z , ' and z ' are the coordinates of the end points ...
... Consider a rod of length Lo at rest parallel to the z ' axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition L1 = z2- z ' , where z , ' and z ' are the coordinates of the end points ...
Page 454
... consider only the electromagnetic aspect . The charge distribution of the atomic nucleus can be crudely approximated by a uniform volume distribution inside a sphere of radius R , falling rapidly to zero outside R. This means that the ...
... consider only the electromagnetic aspect . The charge distribution of the atomic nucleus can be crudely approximated by a uniform volume distribution inside a sphere of radius R , falling rapidly to zero outside R. This means that the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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