Electrodynamics of Continuous Media |
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Page 102
... Let us consider , for example , a contour on the surface of the conductors . When we pass from one conductor to another , the potential has a discontinuity pab . The potential drop across any conductor is RJ , where J is the total ...
... Let us consider , for example , a contour on the surface of the conductors . When we pass from one conductor to another , the potential has a discontinuity pab . The potential drop across any conductor is RJ , where J is the total ...
Page 170
... for a superconductor gik = Sik . Let us now consider multiply - connected superconductors . Their proper- ties are very different from those of simply - connected ones , mainly because it is no longer true that a steady distribution of ...
... for a superconductor gik = Sik . Let us now consider multiply - connected superconductors . Their proper- ties are very different from those of simply - connected ones , mainly because it is no longer true that a steady distribution of ...
Page 231
... us . Let us now consider shock waves in weak magnetic fields , i.e. assume that H2 < pu2 on either side of the discontinuity . No restriction is placed on the discontinuity of any quantity ; in particular , the discontinuity in the ...
... us . Let us now consider shock waves in weak magnetic fields , i.e. assume that H2 < pu2 on either side of the discontinuity . No restriction is placed on the discontinuity of any quantity ; in particular , the discontinuity in the ...
Contents
Notation X | 1 |
2 The energy of the electrostatic field of conductors | 3 |
3 Methods of solving problems in electrostatics | 9 |
Copyright | |
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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 equation div 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 SOLUTION sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic potential tion unit volume values variable velocity wave vector wire z-axis zero