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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 ( 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 H2 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 a д 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 д 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 Bo 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 Bo 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 acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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