Classical Electrodynamics |
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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 ( 1/2 ) ...
... 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 ( 1/2 ) ...
Page 238
... normal outward from the conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written A n д aş 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 A n д aş neglecting the other derivatives when operating on the fields within the conductor . With ...
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ