Electrodynamics of Continuous Media |
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Page 146
... ferromagnetic and ferroelectric phenomena , arising from the difference in the microscopic interaction forces which bring about the spontaneous polarisation . In ferro- electrics , the interaction between the molecules in the crystal ...
... ferromagnetic and ferroelectric phenomena , arising from the difference in the microscopic interaction forces which bring about the spontaneous polarisation . In ferro- electrics , the interaction between the molecules in the crystal ...
Page 152
... ferromagnetic requires a consideration of the shape and size of the body as a whole . We shall return to this ... ferromagnetic . Let us now consider ferromagnetic crystals of the cubic system . Their properties are markedly different ...
... ferromagnetic requires a consideration of the shape and size of the body as a whole . We shall return to this ... ferromagnetic . Let us now consider ferromagnetic crystals of the cubic system . Their properties are markedly different ...
Page 157
... ferromagnetic ellipsoid in an external field H ~ 4πM parallel to one of its axes . The ferromagnetic is assumed to be a cubic crystal . SOLUTION . When the anisotropy energy is neglected , the range for which the domain structure exists ...
... ferromagnetic ellipsoid in an external field H ~ 4πM parallel to one of its axes . The ferromagnetic is assumed to be a cubic crystal . SOLUTION . When the anisotropy energy is neglected , the range for which the domain structure exists ...
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