## Physical Properties of Crystals: Their Representation by Tensors and Matrices |

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Page 54

This is the reason for introducing /AO into equation (2).f Since I refers to

susceptibility. When <ft is positive the substance is said to be paramagnetic;

when ifi is ...

This is the reason for introducing /AO into equation (2).f Since I refers to

**unit****volume**, i/i in equation (2), although dimensionless, is called the volumesusceptibility. When <ft is positive the substance is said to be paramagnetic;

when ifi is ...

Page 149

Their Representation by Tensors and Matrices J. F Nye. Other results. The work

done per

<j, de,. (16) When the change is isothermal and reversible dW may be equated ...

Their Representation by Tensors and Matrices J. F Nye. Other results. The work

done per

**unit volume**when there is a small change of strain in a crystal is dPT =<j, de,. (16) When the change is isothermal and reversible dW may be equated ...

Page 175

Owing to the interplay between the four effects just described, the four differential

coefficients in equations (9) and (10) are not independent. To find the relations

between them we consider the energy of the system. Considering

we ...

Owing to the interplay between the four effects just described, the four differential

coefficients in equations (9) and (10) are not independent. To find the relations

between them we consider the energy of the system. Considering

**unit volume**,we ...

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### Contents

THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |

EQUILIBRIUM PROPERTIES | 51 |

ELECTRIC POLARIZATION | 68 |

15 other sections not shown

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### 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 direction cosines displacement dummy suffix electric field ellipsoid equal equation example expression follows force given heat flow Hence hexagonal homogeneous indicatrix isothermal isotropic left-handed length longitudinal magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optical activity orientation parallel Peltier permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric pyroelectric effect quantities radius vector referred refractive refractive index relation representation quadric represented right-handed rotation scalar second-rank tensor set of axes shear stress suffix notation surface susceptibility symmetry elements Table temperature gradient tensile stress thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law trigonal uniaxial unit volume values written Young's Modulus zero