Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 56
... field and becomes magnetized it sets up a magnetic field of its own , which depends on the susceptibility , the shape , and the size of the crystal . The actual magnetic field acting at any point of space , either inside or outside the ...
... field and becomes magnetized it sets up a magnetic field of its own , which depends on the susceptibility , the shape , and the size of the crystal . The actual magnetic field acting at any point of space , either inside or outside the ...
Page 62
... field . Strictly speaking , the H in equation ( 19 ) is H , while the H in equation ( 20 ) is H. Thus , when the small field H. produced by the crystal itself is taken into account , formula ( 21 ) is not exact . As a result of H even ...
... field . Strictly speaking , the H in equation ( 19 ) is H , while the H in equation ( 20 ) is H. Thus , when the small field H. produced by the crystal itself is taken into account , formula ( 21 ) is not exact . As a result of H even ...
Page 75
... field produced by sources outside the crystal . Owing to the depolarizing effect the force depends on the shape of the specimen , because , in a given external field , the shape affects P. In the para- and diamagnetic case we were able ...
... field produced by sources outside the crystal . Owing to the depolarizing effect the force depends on the shape of the specimen , because , in a given external field , the shape affects P. In the para- and diamagnetic case we were able ...
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