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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 238
... normal outward from the conductor and § is the normal coordinate inward into the conductor , then the gradient operator can be written ~ A -n a 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 a aş neglecting the other derivatives when operating on the fields within the conductor . With ...
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 a ...
... 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 a ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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