Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 191
... isothermal and adiabatic elastic compliances ( at constant field ) proceeds in an exactly analogous way to a calculation of the difference between the heat capacities at constant stress and constant strain ( at constant field ) . A ...
... isothermal and adiabatic elastic compliances ( at constant field ) proceeds in an exactly analogous way to a calculation of the difference between the heat capacities at constant stress and constant strain ( at constant field ) . A ...
Page 202
... isothermal surfaces in this problem may be deduced very directly by using the radius - normal property of the ... isothermal surface . The isothermal surfaces surrounding a point source of heat in an infinite crystal are all similar in ...
... isothermal surfaces in this problem may be deduced very directly by using the radius - normal property of the ... isothermal surface . The isothermal surfaces surrounding a point source of heat in an infinite crystal are all similar in ...
Page 318
... isothermal and adiabatic , 172 , 178 , 186– 8 . matrix equations , 155 , 157 . relations between compliances and stiff- nesses , 147 , 157 . Elasto - optical coefficients , 244 . Electric axis ( quartz ) , 125 . polarization , 68-81 ...
... isothermal and adiabatic , 172 , 178 , 186– 8 . matrix equations , 155 , 157 . relations between compliances and stiff- nesses , 147 , 157 . Elasto - optical coefficients , 244 . Electric axis ( quartz ) , 125 . polarization , 68-81 ...
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