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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 angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ