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 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 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 |
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