Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 82
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 ...
Other editions - View all
Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ