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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 H , 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 H , is much larger than the normal component of H1 , as shown in Fig . 5.10 . In the limit ( u ...
Page 238
... normal outward from the conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written -n a ઠક neglecting the other derivatives when operating on the fields within the conductor . With ...
... normal outward from the conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written -n a ઠક neglecting the other derivatives when operating on the fields within the conductor . With ...
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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