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Page 281
... region I with those in region II boundary conditions for E and B must be satisfied on S , the form of these boundary conditions depending on the properties of S. The method of attack used in solving such problems is the Green's theorem ...
... region I with those in region II boundary conditions for E and B must be satisfied on S , the form of these boundary conditions depending on the properties of S. The method of attack used in solving such problems is the Green's theorem ...
Page 282
... region II . In order to apply the Kirchhoff formula ( 9.65 ) to a diffraction problem it is necessary to know the ... Region I contains the sources of radiation . Region II is the diffraction region , where the fields satisfy the ...
... region II . In order to apply the Kirchhoff formula ( 9.65 ) to a diffraction problem it is necessary to know the ... Region I contains the sources of radiation . Region II is the diffraction region , where the fields satisfy the ...
Page 286
... region II ' . In fact , the hypothetical sources inside the disc will be imagined to be such that the fields in region II ' give a contribution to the surface integral ( 9.77 ) which makes the final expression for the diffracted fields ...
... region II ' . In fact , the hypothetical sources inside the disc will be imagined to be such that the fields in region II ' give a contribution to the surface integral ( 9.77 ) which makes the final expression for the diffracted fields ...
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