Physical Properties of Crystals |
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Page 11
... properties , they are isotropic . All crystals are anisotropic for some of their properties . In this book , then , we study how to specify the physical properties of crystals ; a large number of the properties are represented by ...
... properties , they are isotropic . All crystals are anisotropic for some of their properties . In this book , then , we study how to specify the physical properties of crystals ; a large number of the properties are represented by ...
Page 20
... crystal symmetry on crystal properties We must now leave our discussion of second - rank tensor properties for a while and broaden our outlook to include all crystal properties . We have to examine the question of how the symmetry of a ...
... crystal symmetry on crystal properties We must now leave our discussion of second - rank tensor properties for a while and broaden our outlook to include all crystal properties . We have to examine the question of how the symmetry of a ...
Page 91
... crystal properties We conclude this chapter by pointing out an important distinction between the stress tensor and all the other second - rank tensors so far introduced . Tensors which measure crystal properties ( such as the ...
... crystal properties We conclude this chapter by pointing out an important distinction between the stress tensor and all the other second - rank tensors so far introduced . Tensors which measure crystal properties ( such as the ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
20 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined deformation denoted diad axis dielectric dijk displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ 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 pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress suffixes symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal wave surface x₁ Young's Modulus zero ат