Physical Properties of Crystals |
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Page 14
... set of axes x1 , has three components P , that transform according to equations ( 13 ) . Let us examine this definition more closely ( Eddington 1923 ) . We have three numbers P1 , P2 , P3 which we associate with a certain set of axes ...
... set of axes x1 , has three components P , that transform according to equations ( 13 ) . Let us examine this definition more closely ( Eddington 1923 ) . We have three numbers P1 , P2 , P3 which we associate with a certain set of axes ...
Page 15
... set of axes , the nine coefficients Tij connect the components of two vectors p , and q ; in linear relationships , Pi then , on changing to another set of axes , the T , transform according to equation ( 22 ) , and hence form a second ...
... set of axes , the nine coefficients Tij connect the components of two vectors p , and q ; in linear relationships , Pi then , on changing to another set of axes , the T , transform according to equation ( 22 ) , and hence form a second ...
Page 37
... axes . Consider first the transformation that leaves the axes unchanged , called the identical transformation , ( a1j ) = 1 0 0 = ( Sij ) , 0 1 0 0 - by equation ( 9 ) . In this case evidently | a , ; | = +1 . Now imagine the new set of ...
... axes . Consider first the transformation that leaves the axes unchanged , called the identical transformation , ( a1j ) = 1 0 0 = ( Sij ) , 0 1 0 0 - by equation ( 9 ) . In this case evidently | a , ; | = +1 . Now imagine the new set of ...
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