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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 |
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