## Solid State PhysicsThis book provides an introduction to the field of solid state physics for undergraduate students in physics, chemistry, engineering, and materials science. |

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Page 256

THE THERMOELECTRIC POWER When a

a metal and no electric current is allowed to flow , there will be a steady - state

electrostatic potential difference between the high - and low -

regions ...

THE THERMOELECTRIC POWER When a

**temperature**gradient is maintained ina metal and no electric current is allowed to flow , there will be a steady - state

electrostatic potential difference between the high - and low -

**temperature**regions ...

Page 457

19 ) Jo et Jo Therefore , at very low

. 20 ) OT 10 ( hc ) 3 ( hc ) This relation can be checked by comparing the

measured low -

which ...

19 ) Jo et Jo Therefore , at very low

**temperatures**O T2 ( kBT ) 4 212 , ( KBT ) ( 23. 20 ) OT 10 ( hc ) 3 ( hc ) This relation can be checked by comparing the

measured low -

**temperature**specific heat with the measured elastic constants ,which ...

Page 744

Critical

critical

the density of electronic levels for a single spin population in the normal ...

Critical

**Temperature**In zero magnetic field , superconducting ordering sets in at acritical

**temperature**given by kpt . = 1 . 13hwe - 1 / NoVO , ( 34 . 17 ) where No isthe density of electronic levels for a single spin population in the normal ...

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### Contents

The Drude Theory of Metals | 1 |

Free electron densities and ra | 5 |

Thermal conductivities | 21 |

Copyright | |

46 other sections not shown

### Other editions - View all

Solid State Physics: Advances in Research and Applications, Volume 42 Henry Ehrenreich Limited preview - 1989 |

### Common terms and phrases

additional applied approximation assume atomic band boundary Bragg Bravais lattice calculation carrier Chapter charge close collisions compared completely condition conduction consider constant containing contribution correction crystal cubic density dependence derivation described determined direction discussion distribution effect electric field elements energy equal equation equilibrium example fact Fermi surface Figure follows free electron frequency given gives heat hexagonal holes important independent integral interaction ionic ions known lattice vector leading levels limit linear magnetic field mean measured metals method momentum motion normal Note observed occupied orbits perpendicular phonon plane positive possible potential present primitive cell problem properties reciprocal lattice reflection region relation requires result satisfy scattering semiclassical Show shown simple single solid solution space specific structure symmetry Table temperature term theory thermal vanishes volume wave functions wave vector zero zone