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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 L at rest parallel to the z ′ axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition Loz'z ' , where z , ' and z ' are the coordinates of the end points of the ...
... Consider a rod of length L at rest parallel to the z ′ axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition Loz'z ' , where z , ' and z ' are the coordinates of the end points of the ...
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 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