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

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Page 218

The second law of thermostatics (written as an equality) cannot be applied to the

thermoelectric effects because of the irreversible processes of

and electrical conduction that inevitably accompany them.

The second law of thermostatics (written as an equality) cannot be applied to the

thermoelectric effects because of the irreversible processes of

**heat**conductionand electrical conduction that inevitably accompany them.

**Thomson**proceeded ...Page 229

the temperature gradient; since temperature gradients not in the direction of the

current are relevant now, we have a transverse

normal

the temperature gradient; since temperature gradients not in the direction of the

current are relevant now, we have a transverse

**Thomson heat**, in addition to thenormal

**Thomson heat**. The complete expression for the**Thomson heat**evolved ...Page 322

Joule heat, 204, 217, 221, 226. order of magnitude of effects, 224. Peltier heat,

215, 217-19, 222-3, 226-8. Seebeck effect, 215, 222, 225. thermoelectric power,

217.

Thomson ...

Joule heat, 204, 217, 221, 226. order of magnitude of effects, 224. Peltier heat,

215, 217-19, 222-3, 226-8. Seebeck effect, 215, 222, 225. thermoelectric power,

217.

**Thomson heat**, 215-16, 218, 223, 228-9.**Thomson heat**tensor, 229.Thomson ...

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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