Physical Properties of Crystals |
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Page 11
... quantities , such as the density or the temperature of a body , which are not connected in any way with direction . With the usual definitions of density and temperature it is meaningless to speak of measuring these quantities in any ...
... quantities , such as the density or the temperature of a body , which are not connected in any way with direction . With the usual definitions of density and temperature it is meaningless to speak of measuring these quantities in any ...
Page 21
... quantities , taking our measurements in the same directions as before , relative to the fixed axes . If the relation between the measured quantities is unchanged , we say that the property in question , in this particular crystal ...
... quantities , taking our measurements in the same directions as before , relative to the fixed axes . If the relation between the measured quantities is unchanged , we say that the property in question , in this particular crystal ...
Page 175
... quantities are func- agreed to use to define the state of the itself is a function of ( o ,,, T ) , and therefore ... quantities each contain an arbitrary constant representing the internal energy and the entropy , respectively , in some ...
... quantities are func- agreed to use to define the state of the itself is a function of ( o ,,, T ) , and therefore ... quantities each contain an arbitrary constant representing the internal energy and the entropy , respectively , in some ...
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