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Page 20
... physical interchangeability of the source and the observation points . From form ( 1.40 ) for G ( x , x ' ) it is clear that F ( x , x ' ) is also a symmetric function of its arguments . As a final , important remark we note the physical ...
... physical interchangeability of the source and the observation points . From form ( 1.40 ) for G ( x , x ' ) it is clear that F ( x , x ' ) is also a symmetric function of its arguments . As a final , important remark we note the physical ...
Page 607
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
... physical requirements that ( a ) the normal modes of oscil- lation of the system must decay in time ( even if very slowly ) because of ever - present resistive losses , and ( b ) at high frequencies binding effects are unimportant and ...
Page 620
John David Jackson. Table 4 Conversion - table for given amounts of a physical quantity The table is arranged so that a given amount of some physical quantity , expressed as so many mks or Gaussian units of that quantity , can be ...
John David Jackson. Table 4 Conversion - table for given amounts of a physical quantity The table is arranged so that a given amount of some physical quantity , expressed as so many mks or Gaussian units of that quantity , can be ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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