Electrodynamics of Continuous Media |
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Page 117
... magnetic moment , i.e. the integral frxjdV , again taken over an elementary cell , need not be zero . Accordingly , the bodies for which j # 0 may be divided into two types : those in which the macroscopic magnetic moment is not zero ...
... magnetic moment , i.e. the integral frxjdV , again taken over an elementary cell , need not be zero . Accordingly , the bodies for which j # 0 may be divided into two types : those in which the macroscopic magnetic moment is not zero ...
Page 118
... magnetic properties , the macroscopic symmetry can be classified by groups ( consisting of rotations , reflections ... moment , i.e. of spon- taneous magnetisation in the absence of an external field . The magnetic moment M is a vector ...
... magnetic properties , the macroscopic symmetry can be classified by groups ( consisting of rotations , reflections ... moment , i.e. of spon- taneous magnetisation in the absence of an external field . The magnetic moment M is a vector ...
Page 209
... magnetic field B due to a fixed magnet . We neglect the distortion of the field by the wire itself . According to ... moment of a conducting sphere ( with μ = 1 ) rotating uniformly in a uniform constant magnetic field , and the torque ...
... magnetic field B due to a fixed magnet . We neglect the distortion of the field by the wire itself . According to ... moment of a conducting sphere ( with μ = 1 ) rotating uniformly in a uniform constant magnetic field , and the torque ...
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