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

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Page xiii

A few further examples are : the flow of heat

(thermal conductivity) ; the polarization

(dielectric susceptibility) ; the polarization of a crystal that may be

A few further examples are : the flow of heat

**produced**by a temperature gradient(thermal conductivity) ; the polarization

**produced**in a dielectric by an electric field(dielectric susceptibility) ; the polarization of a crystal that may be

**produced**by ...Page 125

The physical significance of the matrices in Table 8 is best appreciated by

working out the polarization

stress systems. The reader is recommended to do this. We select the

piezoelectric ...

The physical significance of the matrices in Table 8 is best appreciated by

working out the polarization

**produced**in a chosen crystal class by various simplestress systems. The reader is recommended to do this. We select the

piezoelectric ...

Page 171

(ii) A small change of electric field dEt

displacement dDi according to the equation dDt = KtidEi, (2) where Kti is the

permittivity tensor (Ch. IV). (iii) A small change of stress da^

of strain dey ...

(ii) A small change of electric field dEt

**produces**a change of electricdisplacement dDi according to the equation dDt = KtidEi, (2) where Kti is the

permittivity tensor (Ch. IV). (iii) A small change of stress da^

**produces**a changeof strain dey ...

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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