The Degenerate Fermi Gas - Edubirdie

University:
Massachusetts Institute of Technology
Course:
8.333 | Statistical Mechanics I: Statistical Mechanics of Particles
Academic year:

2019
Views:

461

Pages:

3
Author:

prediguemzhv

VII.E The Degenerate Fermi Gas At zero temperature, the fermi occupation number, hn~k i− = 1 , (k)−µ E e +1 (VII.40) β is one for E(~k) < µ, and zero otherwise. The limiting value of µ at zero temperature is called the fermi energy, E F , and all one-particle states of energy less than E F are occupied, forming a fermi sea. For the ideal gas with E(~k) = h̄2 k 2 /(2m), there is a corresponding fermi wavenumber kF , calculated from X N= (2s + 1) = gV |~ k|≤kF Z k

Related Documents

The Degenerate Fermi Gas

The Degenerate Fermi Gas - Page 1

The Degenerate Fermi Gas - Page 2

The Degenerate Fermi Gas - Page 3

of 3

Recommended Documents

The Ideal Gas, Mixing Entropy and Gibbs’ Paradox, the Canonical Ensemble

The Ideal Gas, Mixing Entropy and Gibbs’ Paradox, the Canonical Ensemble

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

Examples, the Gibbs Canonical Ensemble, the Grand Canonical Ensemble

Examples, the Gibbs Canonical Ensemble, the Grand Canonical Ensemble

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

Statistical Mechanics I: Final Exam Review Solution

Statistical Mechanics I: Final Exam Review Solution

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Answer Key

Statistical Mechanics I: Exam Review 3 Solution

Statistical Mechanics I: Exam Review 3 Solution

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Answer Key

Dilute Polyatomic Gases, Vibrations of a Solid, Black-Body Radiation

Dilute Polyatomic Gases, Vibrations of a Solid, Black-Body Radiation

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

The Second Law, Carnot Engines and Thermodynamic Temperature, Entropy

The Second Law, Carnot Engines and Thermodynamic Temperature, Entropy

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

General Definitions, Liouville’s Theorem

General Definitions, Liouville’s Theorem

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

Statistical Mechanics I: Exam Review 1 Solution

Statistical Mechanics I: Exam Review 1 Solution

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Lecture Note

Statistical Mechanics I: Exam Review 2 Solution

Statistical Mechanics I: Exam Review 2 Solution

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Answer Key

8.333 Statistical Mechanics I: Exam Review 2 Solution

8.333 Statistical Mechanics I: Exam Review 2 Solution

Massachusetts Institute of Technology 8.333 | Statistical Mechanics I: Statistical Mechanics of Particles

Answer Key