Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page ix
... Thermodynamics of thermoelastic behaviour 170 173 3. Thermodynamics of thermal , electrical and elastic properties 4. Relations between coefficients measured under different conditions Summary 178 183 191 PART 3. TRANSPORT PROPERTIES XI ...
... Thermodynamics of thermoelastic behaviour 170 173 3. Thermodynamics of thermal , electrical and elastic properties 4. Relations between coefficients measured under different conditions Summary 178 183 191 PART 3. TRANSPORT PROPERTIES XI ...
Page 173
... thermodynamics of the processes must be explored . We shall find that this leads to a precise formula- tion of the properties , and yields a number of new relations between the coefficients defining the properties . 2. Thermodynamics of ...
... thermodynamics of the processes must be explored . We shall find that this leads to a precise formula- tion of the properties , and yields a number of new relations between the coefficients defining the properties . 2. Thermodynamics of ...
Page 175
... thermodynamics that , if a small amount of heat dQ flows into the crystal and a small amount of work dW is done on the crystal by external forces , the increase in the internal energy dU is a perfect differential and is given by dU = dW ...
... thermodynamics that , if a small amount of heat dQ flows into the crystal and a small amount of work dW is done on the crystal by external forces , the increase in the internal energy dU is a perfect differential and is given by dU = dW ...
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