Electrodynamics of continuous mediaVolume 8. |
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Page 61
pyroelectric. We may enumerate those out of the 32 crystal classes in which
triclinic system: C\ monoclinic system : Ct, C2 rhombic system : C2V tetragonal
system : C4, Cnv rhombohedral system : Cz, C$v hexagonal system: Ce, Cgr.
There ...
pyroelectric. We may enumerate those out of the 32 crystal classes in which
triclinic system: C\ monoclinic system : Ct, C2 rhombic system : C2V tetragonal
system : C4, Cnv rhombohedral system : Cz, C$v hexagonal system: Ce, Cgr.
There ...
Page 84
the spontaneous polarisation is then determined apart from sign, since in the non
-pyroelectric phase the two opposite directions parallel to the ferroelectric axis
must be entirely equivalent (otherwise this form of the crystal would also be ...
the spontaneous polarisation is then determined apart from sign, since in the non
-pyroelectric phase the two opposite directions parallel to the ferroelectric axis
must be entirely equivalent (otherwise this form of the crystal would also be ...
Page 86
{T—&)\ but for sufficiently large values of Ez we have Dz = {EzjB.y. The
proportionality coefficient ete> in the linear relation is the dielectric constant of the
non-pyroelectric phase. For T -*. 0 it increases without limit in inverse proportion
to T— 0, ...
{T—&)\ but for sufficiently large values of Ez we have Dz = {EzjB.y. The
proportionality coefficient ete> in the linear relation is the dielectric constant of the
non-pyroelectric phase. For T -*. 0 it increases without limit in inverse proportion
to T— 0, ...
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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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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 curlH current density cylinder denote depends derivative determined dielectric permeability difference differentiating diffraction dipole direction discontinuity distance e(to effect electric field electromagnetic electrons electrostatic ellipsoid entropy equation expression external field external magnetic field ferroelectric ferromagnetic fluid flux force formula free energy frequency function given gives grad Hence induction integral isotropic Laplace's equation layer Let us consider linear macroscopic magnetic field magnetisation magnitude Maxwell's equations medium metal normal obtain optical particle perpendicular phase piezoelectric plane polarisation Problem propagation properties pyroelectric quantities radius refraction relation respect result rotation scalar scattering self-inductance Solution sphere suffixes superconducting surface symmetry tangential temperature theory thermodynamic equilibrium thermodynamic potential tion uniform unit volume values variable velocity wave vector wire zero