Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 53
Their Representation by Tensors and Matrices John Frederick Nye. III PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY THE magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented ...
Their Representation by Tensors and Matrices John Frederick Nye. III PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY THE magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented ...
Page 54
... susceptibility . When is positive the substance is said to be para- magnetic ; when is negative it is diamagnetic . Although is dimensionless , as defined here , the numerical value of the volume susceptibility for a given substance ...
... susceptibility . When is positive the substance is said to be para- magnetic ; when is negative it is diamagnetic . Although is dimensionless , as defined here , the numerical value of the volume susceptibility for a given substance ...
Page 66
... susceptibility of a powder If a powder consisting of randomly oriented anisotropic crystal grains is placed in a ... susceptibility directions is given by μo ¥ H = μo ( 41l3 + 4213 + 4,13 ) H , where is the susceptibility in the ( 11 ...
... susceptibility of a powder If a powder consisting of randomly oriented anisotropic crystal grains is placed in a ... susceptibility directions is given by μo ¥ H = μo ( 41l3 + 4213 + 4,13 ) H , where is the susceptibility in the ( 11 ...
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