Physical Properties of Crystals: Their Representation by Tensors and Matrices |
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Page 53
... magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented by a second - rank tensor . In this chapter we first formulate the property , and then show how the formulation leads ...
... magnetic susceptibility of paramagnetic and diamagnetic crystals is a typical anisotropic crystal property represented by a second - rank tensor . In this chapter we first formulate the property , and then show how the formulation leads ...
Page 60
... magnetic field . Suppose a magnetic dipole of strength M is situated in a uniform magnetic field of intensity H so that the direction of the dipole makes an angle 0 with the direction of H ( Fig . 3.4 ) . The dipole may be imagined to ...
... magnetic field . Suppose a magnetic dipole of strength M is situated in a uniform magnetic field of intensity H so that the direction of the dipole makes an angle 0 with the direction of H ( Fig . 3.4 ) . The dipole may be imagined to ...
Page 70
... magnetic poles are an artificial concept , although a convenient one . A physically realistic approach would recognize from the beginning the common origin of both magnetic and electric fields . It would regard magnetic fields and ...
... magnetic poles are an artificial concept , although a convenient one . A physically realistic approach would recognize from the beginning the common origin of both magnetic and electric fields . It would regard magnetic fields and ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ 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 produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт