Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 66
Page 82
... stress A BODY which is acted on by external forces , or , more generally , a body in which one part exerts a force on neighbouring parts , is said to be in a state of stress . If we consider a volume element situated within a stressed ...
... stress A BODY which is acted on by external forces , or , more generally , a body in which one part exerts a force on neighbouring parts , is said to be in a state of stress . If we consider a volume element situated within a stressed ...
Page 90
... stress axes , σ = 4. Special forms of the stress tensor We give now some of the forms taken by the stress tensor , referred to its principal axes , in special cases . ( i ) Uniaxial stress , o . σ 0 01 0 0 0 0 An example is the stress ...
... stress axes , σ = 4. Special forms of the stress tensor We give now some of the forms taken by the stress tensor , referred to its principal axes , in special cases . ( i ) Uniaxial stress , o . σ 0 01 0 0 0 0 An example is the stress ...
Page 131
... stress . Provided the stress is below a certain limiting value , the elastic limit , the strain is recoverable , that is to say , the body returns to its original shape when the stress is removed . It is further observed ( Hooke's Law ) ...
... stress . Provided the stress is below a certain limiting value , the elastic limit , the strain is recoverable , that is to say , the body returns to its original shape when the stress is removed . It is further observed ( Hooke's Law ) ...
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