Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 47
Page 33
... angles are necessary to specify the direction of Ox1 , the latitude and longitude for example ; the new axes may still rotate about Oxí , and so one further angle , an angle of rotation about Ox1 , is needed to fix them completely ...
... angles are necessary to specify the direction of Ox1 , the latitude and longitude for example ; the new axes may still rotate about Oxí , and so one further angle , an angle of rotation about Ox1 , is needed to fix them completely ...
Page 97
... angle between them after deformation is 7-212 ( centre diagram of Fig . 6.6 ) . Note particularly that the tensor shear strain 12 is one - half of the change in angle between the two elements . 2.1 . Homogeneous two - dimensional strain ...
... angle between them after deformation is 7-212 ( centre diagram of Fig . 6.6 ) . Note particularly that the tensor shear strain 12 is one - half of the change in angle between the two elements . 2.1 . Homogeneous two - dimensional strain ...
Page 109
... angles between the principal expansion directions and Oz . Illustrate the answer by a Mohr circle diagram ( compare the ... angle ( 001 ) : ( 011 ) increases by 2 · 84 ' . The coefficient of bulk expansion is 62.0 × 10 − ❝ per C ...
... angles between the principal expansion directions and Oz . Illustrate the answer by a Mohr circle diagram ( compare the ... angle ( 001 ) : ( 011 ) increases by 2 · 84 ' . The coefficient of bulk expansion is 62.0 × 10 − ❝ per C ...
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