Physical Properties of Crystals |
From inside the book
Results 1-3 of 28
Page 119
... moduli one by one , and transform them according to ( 23 ) . If the sign changes the modulus must be zero ; if the ... moduli are therefore those in bold type in the array : d111 d112 d113 d122 d123 d133 d211 d212 d213 d222 d223 d233 ...
... moduli one by one , and transform them according to ( 23 ) . If the sign changes the modulus must be zero ; if the ... moduli are therefore those in bold type in the array : d111 d112 d113 d122 d123 d133 d211 d212 d213 d222 d223 d233 ...
Page 120
... moduli having no 3's or two 3's . Hence a diad parallel to x1 removes all moduli having no 1's or two l's . There- fore , only the following moduli remain , d123 = d213 , In the two suffix notation these are d14 = d25 , d312 ( = d321 ) ...
... moduli having no 3's or two 3's . Hence a diad parallel to x1 removes all moduli having no 1's or two l's . There- fore , only the following moduli remain , d123 = d213 , In the two suffix notation these are d14 = d25 , d312 ( = d321 ) ...
Page 122
... moduli are derived in a straightforward way and are found to be , for a 3 - fold or a 6 - fold axis , d113d223 , d123 = -d213 , d311 d133 = d233 - d312d313 = d322 , = d323 = 0 . We have thus found the conditions on the moduli for ...
... moduli are derived in a straightforward way and are found to be , for a 3 - fold or a 6 - fold axis , d113d223 , d123 = -d213 , d311 d133 = d233 - d312d313 = d322 , = d323 = 0 . We have thus found the conditions on the moduli for ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 11 |
EQUILIBRIUM PROPERTIES | 45 |
PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY | 53 |
20 other sections not shown
Common terms and phrases
angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined deformation denoted diad axis dielectric dijk displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ 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 pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress suffixes symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal wave surface x₁ Young's Modulus zero ат