Classical ElectrodynamicsProblems after each chapter |
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Page 174
... consider these contributions . Suppose for a moment that we have only a single circuit with a constant current I flowing in it . If the flux through the circuit changes , an electro- motive force & is induced around it . In order to ...
... consider these contributions . Suppose for a moment that we have only a single circuit with a constant current I flowing in it . If the flux through the circuit changes , an electro- motive force & is induced around it . In order to ...
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 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 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ