Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page xiii
... cubic crystals are anisotropic , often markedly so , for elasticity , photoelasticity , and certain other properties . We must therefore regard cubic crystals as potentially anisotropic , and then we can go on to INTRODUCTION.
... cubic crystals are anisotropic , often markedly so , for elasticity , photoelasticity , and certain other properties . We must therefore regard cubic crystals as potentially anisotropic , and then we can go on to INTRODUCTION.
Page 147
... cubic system the linear compressibility is isotropic : a sphere of a cubic crystal under hydrostatic pressure remains a sphere . EXERCISE 8.2 . Prove that the volume change of a cubic crystal under uni- axial tension T is independent of ...
... cubic system the linear compressibility is isotropic : a sphere of a cubic crystal under hydrostatic pressure remains a sphere . EXERCISE 8.2 . Prove that the volume change of a cubic crystal under uni- axial tension T is independent of ...
Page 254
... cubic crystals are given Tij in Table 17. The values are sometimes slightly dependent on the wave- length of the light . Care is needed with the signs . † To illustrate the signs suppose that a crystal of sodium chloride is compressed ...
... cubic crystals are given Tij in Table 17. The values are sometimes slightly dependent on the wave- length of the light . Care is needed with the signs . † To illustrate the signs suppose that a crystal of sodium chloride is compressed ...
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