## Physical Properties of Crystals |

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Page 153

A further point of manipulation where matrices A, B differ from ordinary numbers a

, b is that, whereas the equation ab = 0 implies that either a or b (or both) is

the equation AB = 0 (0 standing for the null matriz all of whose elements are ...

A further point of manipulation where matrices A, B differ from ordinary numbers a

, b is that, whereas the equation ab = 0 implies that either a or b (or both) is

**zero**,the equation AB = 0 (0 standing for the null matriz all of whose elements are ...

Page 185

It can be seen from this diagram that, if the conditions were such that P was

always perpendicular to the surfaces, D would always be

depolarizing field caused by the surface polarization charges, would then always

be such ...

It can be seen from this diagram that, if the conditions were such that P was

always perpendicular to the surfaces, D would always be

**zero**; E, which is adepolarizing field caused by the surface polarization charges, would then always

be such ...

Page 211

One of the consequences of not accepting (4) would be that we should have to

assume that the conductivity of a vacuum is not

surface of a crystal perpendicular to aca. In the crystal, if (4) is not accepted, we

have ...

One of the consequences of not accepting (4) would be that we should have to

assume that the conductivity of a vacuum is not

**zero**. To see this, take a flatsurface of a crystal perpendicular to aca. In the crystal, if (4) is not accepted, we

have ...

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### Contents

THE GROUND WORK OF CRYSTAL PHYSICS | 3 |

Summary | 29 |

EQUILIBRIUM PROPERTIES | 45 |

47 other sections not shown

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### Common terms and phrases

angle anisotropic applied biaxial birefringence centre of symmetry Chapter conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals defined denoted diad axis dielectric direction cosines displacement elastic compliances electric field electro-optical electro-optical effect ellipsoid equal equation example expression follows forces given gives grad heat flow Hence indicatrix isothermal isotropic magnetic magnitude matrix notation measured moduli Mohr circle monoclinic number of independent Onsager's Principle optic axis optical activity orientation parallel permittivity perpendicular photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation scalar second-rank tensor shear shown shows strain stress 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