Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 202
... similar result would not apply to the temperature gradient vectors , for they are in both cases perpen- dicular to ... similar to an isothermal surface . The isothermal surfaces surrounding a point source of heat in an infinite crystal ...
... similar result would not apply to the temperature gradient vectors , for they are in both cases perpen- dicular to ... similar to an isothermal surface . The isothermal surfaces surrounding a point source of heat in an infinite crystal ...
Page 248
... similar to that used in dealing with the elastic compliances ( pp . 132-3 ) . The relations ( 21 ) and ( 22 ) reduce the number of independent coeffi- cients from 34 = 81 to 36 , and they make possible a similar abbreviated notation to ...
... similar to that used in dealing with the elastic compliances ( pp . 132-3 ) . The relations ( 21 ) and ( 22 ) reduce the number of independent coeffi- cients from 34 = 81 to 36 , and they make possible a similar abbreviated notation to ...
Page 307
... similar equations . Hence and two similar equations . - K1 Di = ( 1.E ) Мога - 0 , = D1 / K1 etc. , ( 15 ) Since D is normal to 1 , the scalar product D.1 vanishes . We now express this product in terms of the components of D given by ...
... similar equations . Hence and two similar equations . - K1 Di = ( 1.E ) Мога - 0 , = D1 / K1 etc. , ( 15 ) Since D is normal to 1 , the scalar product D.1 vanishes . We now express this product in terms of the components of D given by ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
EQUILIBRIUM PROPERTIES | 51 |
ELECTRIC POLARIZATION | 68 |
18 other sections not shown
Common terms and phrases
angle anisotropic applied axial vector centre of symmetry Chapter coefficients conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric dijk direction cosines dummy suffix elastic electric field ellipsoid equation example force given grad H₁ H₂ heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive index relation representation quadric represented right-handed rotation S₁ scalar second-rank tensor set of axes shear strain stress suffix notation surface susceptibility symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values x₁ Young's Modulus zero