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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 = Σ x v1 ) ( 5.62 ) The vector product ( x , x Li angular momentum , L1 = 2c v1 ) is proportional to the ith particle's orbital M1 ( x , x v1 ) . Thus ( 5.62 ) becomes qi Li m = 2M , c ( 5.63 ) If all the particles in motion ...
... becomes m = Σ x v1 ) ( 5.62 ) The vector product ( x , x Li angular momentum , L1 = 2c v1 ) is proportional to the ith particle's orbital M1 ( x , x v1 ) . Thus ( 5.62 ) becomes qi Li m = 2M , c ( 5.63 ) If all the particles in motion ...
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 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ