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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 171
... physical laws should be invariant under Galilean transformations . That is , physical phenomena are the same when viewed by two observers moving with a constant velocity v relative to one another , provided the coordinates in space and ...
... physical laws should be invariant under Galilean transformations . That is , physical phenomena are the same when viewed by two observers moving with a constant velocity v relative to one another , provided the coordinates in space and ...
Page
... 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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