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 227
... , through equation ( 44 ) , the existence of a transverse Peltier effect that is peculiar to non- cubic crystals . This may be seen by considering a rod of non - cubic crystal ( Fig . 12.2 ) with its length parallel § 3 227 ...
... , through equation ( 44 ) , the existence of a transverse Peltier effect that is peculiar to non- cubic crystals . This may be seen by considering a rod of non - cubic crystal ( Fig . 12.2 ) with its length parallel § 3 227 ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ heat flow Hence hexagonal indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт