## Introduction to Solid State Physicsproblems after each chapter |

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Page 138

... heat capacity of 1 gm of a suitable paramagnetic salt may be comparable with

that of 1 ton of a non - magnetic salt . It is obvious that paramagnetic impurities

must be carefully guarded against in

.

... heat capacity of 1 gm of a suitable paramagnetic salt may be comparable with

that of 1 ton of a non - magnetic salt . It is obvious that paramagnetic impurities

must be carefully guarded against in

**thermal**measurements at low temperatures.

Page 139

where Q is the flux of

unit time ) ; K is often expressed in units cal / cm - sec - deg or watts / cm - deg .

To convert to watts / cm - deg , multiply K in cal / cmsec - deg by 4 . 186 . The form

of ...

where Q is the flux of

**thermal**energy ( energy transmitted across unit area perunit time ) ; K is often expressed in units cal / cm - sec - deg or watts / cm - deg .

To convert to watts / cm - deg , multiply K in cal / cmsec - deg by 4 . 186 . The form

of ...

Page 151

Al

Mn 39 % MnXSARA E11 24 % NiX dom ex 31 % Ni 1 3 % Cr , quenched 36 %

Nior . 19 % Cr X A13 % Mn , 1 % Crvene 27 % Nior IM * 10 20 40 60 80 100 200

...

Al

**Thermal**conductivity ( milliwatts / cm deg k ) 77 X 2 % Mn Xr57 % Ni / / 13 %Mn 39 % MnXSARA E11 24 % NiX dom ex 31 % Ni 1 3 % Cr , quenched 36 %

Nior . 19 % Cr X A13 % Mn , 1 % Crvene 27 % Nior IM * 10 20 40 60 80 100 200

...

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### Contents

DIFFRACTION OF XRAYS BY CRYSTALS | 44 |

CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |

ELASTIC CONSTANTS OF CRYSTALS | 85 |

Copyright | |

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### Common terms and phrases

alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential present problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone