Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 113
... independent components the coefficients shown in brackets , leaving 18 independent dijk ; it also facilitates the use of a more concise notation known as the matrix notation . Up to this point all the equations have been developed in ...
... independent components the coefficients shown in brackets , leaving 18 independent dijk ; it also facilitates the use of a more concise notation known as the matrix notation . Up to this point all the equations have been developed in ...
Page 122
... independent , but only the total number of independent ones . The listing of the independent components in each class by group theoretical methods has been studied by Fumi ( 1952d ) and by Fieschi and Fumi ( 1953 ) , who give further ...
... independent , but only the total number of independent ones . The listing of the independent components in each class by group theoretical methods has been studied by Fumi ( 1952d ) and by Fieschi and Fumi ( 1953 ) , who give further ...
Page 293
Their Representation by Tensors and Matrices John Frederick Nye. APPENDIX D THE NUMBER OF INDEPENDENT COEFFICIENTS IN THE 32 CRYSTAL CLASSES IN Table 25 , p . 294 , are listed , for each of the 32 crystal classes , the number of independent ...
Their Representation by Tensors and Matrices John Frederick Nye. APPENDIX D THE NUMBER OF INDEPENDENT COEFFICIENTS IN THE 32 CRYSTAL CLASSES IN Table 25 , p . 294 , are listed , for each of the 32 crystal classes , the number of independent ...
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