Physical Properties of Crystals |
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Page 11
... produced by a temperature gradient ( thermal con- ductivity ) ; the polarization produced in a dielectric by an electric field ( dielectric susceptibility ) ; the polarization of a crystal that may be produced by mechanical stress ...
... produced by a temperature gradient ( thermal con- ductivity ) ; the polarization produced in a dielectric by an electric field ( dielectric susceptibility ) ; the polarization of a crystal that may be produced by mechanical stress ...
Page 57
... produce a given change in the magnetization of a body can depend on how this change is produced . We shall show below ( for a special case ) that if the change is brought about while the field is maintained by the current in a solenoid ...
... produce a given change in the magnetization of a body can depend on how this change is produced . We shall show below ( for a special case ) that if the change is brought about while the field is maintained by the current in a solenoid ...
Page 125
... produced in a chosen crystal class by various simple stress systems . The reader is recommended to do this . We select the piezoelectric behaviour of quartz , which is of considerable practical importance , for more detailed study ...
... produced in a chosen crystal class by various simple stress systems . The reader is recommended to do this . We select the piezoelectric behaviour of quartz , which is of considerable practical importance , for more detailed study ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
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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