Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 68
Their Representation by Tensors and Matrices John Frederick Nye. IV ELECTRIC POLARIZATION THE polarization of a crystal produced by an electric field is another example of an anisotropic crystal property that is represented by a second ...
Their Representation by Tensors and Matrices John Frederick Nye. IV ELECTRIC POLARIZATION THE polarization of a crystal produced by an electric field is another example of an anisotropic crystal property that is represented by a second ...
Page 81
... polarization between these temperatures . ) A crystal in its ferroelectric state , with a spontaneous polarization , must be of lower symmetry than the same crystal in its non - polar state , and must belong to one of the classes that ...
... polarization between these temperatures . ) A crystal in its ferroelectric state , with a spontaneous polarization , must be of lower symmetry than the same crystal in its non - polar state , and must belong to one of the classes that ...
Page 125
... polarization produced in a chosen crystal class by various simple stress systems . The reader is recommended to do ... polarization are given by the moduli in the first column of the matrix ; thus P1 = d111 , P2 = 0 , P = 0 . X , X У X2 ...
... polarization produced in a chosen crystal class by various simple stress systems . The reader is recommended to do ... polarization are given by the moduli in the first column of the matrix ; thus P1 = d111 , P2 = 0 , P = 0 . X , X У X2 ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero