## Solid state physics |

### From inside the book

Results 1-3 of 12

Page 94

It does not depend on A or L, the dimensions of the

property of the metal itself. Its value is different for each type of metal. The

conductivity of a number of metals is given in Appendix 4. (Some tables give the

resistivity ...

It does not depend on A or L, the dimensions of the

**wire**. The conductivity is aproperty of the metal itself. Its value is different for each type of metal. The

conductivity of a number of metals is given in Appendix 4. (Some tables give the

resistivity ...

Page 274

Note that only non-magnetic metals can exhibit superconductivity. 13-2 Trapped

Magnetic Flux and Persistent Currents Let us discuss some of the unusual

properties of superconductors. Consider a loop of

exhibits ...

Note that only non-magnetic metals can exhibit superconductivity. 13-2 Trapped

Magnetic Flux and Persistent Currents Let us discuss some of the unusual

properties of superconductors. Consider a loop of

**wire**made of a metal whichexhibits ...

Page 281

Consider a solenoid of copper

(This solenoid would be wound about 10 layers thick.) The diameter of the

solenoid is 10 cm and its length is 20 cm. How much current would be required to

...

Consider a solenoid of copper

**wire**, 1.00 mm in diameter, with 100 winds per cm.(This solenoid would be wound about 10 layers thick.) The diameter of the

solenoid is 10 cm and its length is 20 cm. How much current would be required to

...

### What people are saying - Write a review

We haven't found any reviews in the usual places.

### Contents

XRay Diffraction | 37 |

Lattice Vibrations | 61 |

Classical Model of Metals | 89 |

Copyright | |

12 other sections not shown

### Common terms and phrases

Answer Appendix basis vectors bcc lattice bond Bragg angle Bragg's Law Bravais lattice Brillouin zone called Chapter collisions conduction electrons Consider conventional unit cell Cooper pairs depletion layer diode direction dispersion curve displacement distance doped effective mass elec electric current electric field electrons and holes emitter energy band equal example Fermi energy Fermi level Fermi surface force forward biased free electron free particle frequency given by Eq inside integers ions k-space laser lattice parameter lattice points lattice vector lattice wave magnetic field n-type semiconductor NaCl negative neutrons number of electrons obtain occupied one-dimensional oscillate p-n junction photon positively charged potential energy primitive unit cell Problem rays reciprocal lattice reverse biased sc lattice scattered Schroedinger's equation shown in Fig sodium metal solid structure superconductor temperature tion transistor trons unit cell unoccupied values velocity voltage wave function wave number wave vector wavelength Wigner-Seitz cell wire x-ray diffraction zero