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Page 177
... condition of equilibrium which must be fulfilled at every point of a surface ... boundary conditions on the magnetic field and the conditions of thermo ... boundary between these parts is Her . Thus the surface of separation , on which H ...
... condition of equilibrium which must be fulfilled at every point of a surface ... boundary conditions on the magnetic field and the conditions of thermo ... boundary between these parts is Her . Thus the surface of separation , on which H ...
Page 190
... boundary condition ( 45.8 ) shows that the magnetic field in the conductor is also Hoe - iwt at the surface . = We take the surface of the conductor as the xy - plane , the conducting medium being in > 0. Since the conditions of the ...
... boundary condition ( 45.8 ) shows that the magnetic field in the conductor is also Hoe - iwt at the surface . = We take the surface of the conductor as the xy - plane , the conducting medium being in > 0. Since the conditions of the ...
Page 296
... boundary condition ƒ = 0 , the only solution of this equation regular throughout the cross - section ( whether or not multiply connected ) is f = 0. Hence we have E2 = 0 in a principal wave . Ez With the boundary condition of an = 0 , a ...
... boundary condition ƒ = 0 , the only solution of this equation regular throughout the cross - section ( whether or not multiply connected ) is f = 0. Hence we have E2 = 0 in a principal wave . Ez With the boundary condition of an = 0 , a ...
Contents
ELECTROSTATICS OF CONDUCTORS 1 The electrostatic field of conductors | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
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Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
angle anisotropy atoms averaging axes axis body boundary condition calculated charge circuit co-ordinates coefficient components conducting conductor constant corresponding cross-section crystal Curie point curl H current density cylinder denote depends derivative determined dielectric permeability diffraction dipole direction discontinuity distance effect electric field electromagnetic electrons electrostatic ellipsoid entropy expression external field ferroelectric ferromagnetic field H fluid flux force formula free energy frequency function given gives grad H₂ Hence incident induction integral isotropic Laplace's equation layer linear macroscopic magnetic field magnetic moment magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular piezoelectric plane polarisation PROBLEM propagation properties pyroelectric quantities refraction relation respect result rotation scalar scattering self-inductance SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion uniform unit volume values variable velocity wave vector wire z-axis zero