Physical Properties of Crystals |
From inside the book
Results 1-3 of 32
Page 53
John Frederick Nye. III PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY THE magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented by a second - rank tensor . In this chapter we ...
John Frederick Nye. III PARAMAGNETIC AND DIAMAGNETIC SUSCEPTIBILITY THE magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented by a second - rank tensor . In this chapter we ...
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 Можн = Mo ( 4112 + 4212 + 4313 ) H , where is the susceptibility in the ( 11 , 12 ...
... susceptibility of a powder If a powder consisting of randomly oriented anisotropic crystal grains is placed in a ... susceptibility directions is given by Можн = Mo ( 4112 + 4212 + 4313 ) H , where is the susceptibility in the ( 11 , 12 ...
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