Classical Electrodynamics |
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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 ∞ 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 ∞ 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 Lo = zą z'z ' , where z1 ' and z2 are the coordinates of the end points of ...
... 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 Lo = zą z'z ' , where z1 ' and z2 are the coordinates of the end points of ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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