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

### From inside the book

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Page 56

These are, of course, subject to any restrictions that the symmetry of the crystal

may impose (see

diamagnetic along a particular one of the principal axes if tfi for that direction is

respectively ...

These are, of course, subject to any restrictions that the symmetry of the crystal

may impose (see

**Table**3, p. 23). A crystal is said to be paramagnetic ordiamagnetic along a particular one of the principal axes if tfi for that direction is

respectively ...

Page 249

The forms of the (77m„) matrices are given in

which is similar to that already introduced, appears at the head of the

usual, we use the standard setting of the reference axes in relation to the

symmetry ...

The forms of the (77m„) matrices are given in

**Table**15. A key to the notation,which is similar to that already introduced, appears at the head of the

**table**. Asusual, we use the standard setting of the reference axes in relation to the

symmetry ...

Page 291

Notes on

variables shown in the defining equations holds only for sufficiently small values

of the variables. For larger values a differential definition is adopted, for example,

...

Notes on

**Tables**22 a and 226 (1) The simple proportionality between thevariables shown in the defining equations holds only for sufficiently small values

of the variables. For larger values a differential definition is adopted, for example,

...

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### Contents

THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |

EQUILIBRIUM PROPERTIES | 51 |

ELECTRIC POLARIZATION | 68 |

69 other sections not shown

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### Common terms and phrases

angle anisotropic applied biaxial birefringence centre of symmetry Chapter coefficients conductivity crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dijk direction cosines electric field electro-optical effect ellipsoid equal equation example expression follows force given gives heat flow Hence hexagonal indicatrix isothermal isotropic lattice left-handed magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation permittivity perpendicular photoelastic effect piezoelectric effect plane plate point group positive principal axes produced pyroelectric effect quadric quantities radius vector referred refractive index relation representation quadric represents right-handed rotation scalar second-rank tensor set of axes shear shown shows strain stress suffix notation symbol symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law trigonal uniaxial unit volume values wave normal wave surface written zero