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Page 46
... becomes infinite , the set of orthogonal functions U ( ) 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 U ( ) 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 = 2c ( 5.62 ) The vector product ( x ; × v1 ) is proportional to the ith particle's orbital angular momentum , L1 = M , ( x , x v . ) . Thus ( 5.62 ) becomes qi m = Li 2M , c ( 5.63 ) If all the particles in motion have the ...
... becomes m = 2c ( 5.62 ) The vector product ( x ; × v1 ) is proportional to the ith particle's orbital angular momentum , L1 = M , ( x , x v . ) . Thus ( 5.62 ) becomes qi m = Li 2M , c ( 5.63 ) If all the particles in motion have 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.
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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