Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 28
Page 21
... homogeneous stress and a homogeneous strain in the crystal . Now suppose we wish to know whether a property has a certain sym- metry element or not . First we measure the property relative to some fixed axes . Then we operate with the ...
... homogeneous stress and a homogeneous strain in the crystal . Now suppose we wish to know whether a property has a certain sym- metry element or not . First we measure the property relative to some fixed axes . Then we operate with the ...
Page 98
Their Representation by Tensors and Matrices John Frederick Nye. 2.1 . Homogeneous two - dimensional strain . When the distortion is homogeneous the e ;; components are all constants and equations ( 3 ) integrate to Ui = ( u ) ; + еjx ...
Their Representation by Tensors and Matrices John Frederick Nye. 2.1 . Homogeneous two - dimensional strain . When the distortion is homogeneous the e ;; components are all constants and equations ( 3 ) integrate to Ui = ( u ) ; + еjx ...
Page 131
... homogeneous stress and a homogeneous strain are each specified , in general , by second - rank tensors . It is found that , if a general homogeneous stress σ , is applied to a crystal , the resulting homogeneous strain Eij is such that ...
... homogeneous stress and a homogeneous strain are each specified , in general , by second - rank tensors . It is found that , if a general homogeneous stress σ , is applied to a crystal , the resulting homogeneous strain Eij is such that ...
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