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Page 46
... becomes infinite , the set of orthogonal functions Un ( ) may become a continuum of functions , rather than a denumerable set . Then the Kronecker delta symbol in ( 2.35 ) becomes a Dirac delta function . An important example is the ...
... becomes infinite , the set of orthogonal functions Un ( ) may become a continuum of functions , rather than a denumerable set . Then the Kronecker delta symbol in ( 2.35 ) becomes a Dirac delta function . An important example is the ...
Page 148
... becomes m = ` q1 ( x , × v1 ) 2c ( 5.62 ) The vector product ( x , x v1 ) is proportional to the ith particle's orbital angular momentum , L , M. ( x , x v1 ) . Thus ( 5.62 ) becomes = qi Li m = Sai 2M , c ( 5.63 ) = If all the ...
... becomes m = ` q1 ( x , × v1 ) 2c ( 5.62 ) The vector product ( x , x v1 ) is proportional to the ith particle's orbital angular momentum , L , M. ( x , x v1 ) . Thus ( 5.62 ) becomes = qi Li m = Sai 2M , c ( 5.63 ) = If all the ...
Page 310
... , the electrostatic restoring forces become so weak that the length scale of charge separation becomes large compared to the size of the volume being considered . Then the collective behavior implicit in 310 Classical Electrodynamics.
... , the electrostatic restoring forces become so weak that the length scale of charge separation becomes large compared to the size of the volume being considered . Then the collective behavior implicit in 310 Classical Electrodynamics.
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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