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Page 9
... normal to S , and the path C is traversed in a right - hand screw sense relative to n ] leads immediately back to V x E = 0 . 1.6 Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One ...
... normal to S , and the path C is traversed in a right - hand screw sense relative to n ] leads immediately back to V x E = 0 . 1.6 Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One ...
Page 155
... normal n ' parallel to the interface and surface S , Stokes's theorem can be applied to the curl equation in ( 5.84 ) ... normal component of H2 is much larger than the normal component of H1 , as shown in Fig . 5.10 . In the limit ( u ...
... normal n ' parallel to the interface and surface S , Stokes's theorem can be applied to the curl equation in ( 5.84 ) ... normal component of H2 is much larger than the normal component of H1 , as shown in Fig . 5.10 . In the limit ( u ...
Page 298
... normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E , and B。 occur only in a region with dimensions small compared to ...
... normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E , and B。 occur only in a region with dimensions small compared to ...
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