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Page 46
... becomes infinite , the set of orthogonal functions U1 ( § ) 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 U1 ( § ) 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 • Σ9 , ( x , x v1 ) i ( 5.62 ) The vector product ( x , x v1 ) is proportional to the ith particle's orbital angular momentum , L , M , ( x , x v ) . Thus ( 5.62 ) becomes = m = qi Li 2M , c ( 5.63 ) If all the particles ...
... becomes m = 2c • Σ9 , ( x , x v1 ) i ( 5.62 ) The vector product ( x , x v1 ) is proportional to the ith particle's orbital angular momentum , L , M , ( x , x v ) . Thus ( 5.62 ) becomes = m = qi Li 2M , c ( 5.63 ) If all the particles ...
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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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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