## Introduction to Solid State Physics |

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Page 36

We compare the calculated Coulomb energy with the

energy , and then estimate n on the basis of Eq . ( 2 . 5 ) . U ( Coulomb ) U . (

NaI 180 ...

We compare the calculated Coulomb energy with the

**observed**total bindingenergy , and then estimate n on the basis of Eq . ( 2 . 5 ) . U ( Coulomb ) U . (

**observed**) Substance ( kcal / mole ) ( kcal / mole ) NaCl 206 183 NaBr 195 173NaI 180 ...

Page 266

9 shows that the Grüneisen relation works quite well for the metals indicated

there ; at quite low temperatures , however , departures from the TTM law are

usually

conductivity of ...

9 shows that the Grüneisen relation works quite well for the metals indicated

there ; at quite low temperatures , however , departures from the TTM law are

usually

**observed**. Reference to detailed theoretical calculations of theconductivity of ...

Page 297

Thus we estimate for the critical shear stress ( 16 . 2 ) Oc ~ G / 4 . From values of

044 given in Table 3 . 1 we may expect the critical shear stress to be of the order

of 1010 to 1011 dynes / cm2 . The

Thus we estimate for the critical shear stress ( 16 . 2 ) Oc ~ G / 4 . From values of

044 given in Table 3 . 1 we may expect the critical shear stress to be of the order

of 1010 to 1011 dynes / cm2 . The

**observed**shearing stress required ...### What people are saying - Write a review

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### Contents

LATTICE ENERGY OF IONIC CRYSTALS | 29 |

ELASTIC CONSTANTS OF CRYSTALS | 43 |

LATTICE VIBRATIONS | 60 |

Copyright | |

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alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero