Statistical MechanicsUnlike most other texts on the subject, this clear, concise introduction to the theory of microscopic bodies treats the modern theory of critical phenomena. Provides up-to-date coverage of recent major advances, including a self-contained description of thermodynamics and the classical kinetic theory of gases, interesting applications such as superfluids and the quantum Hall effect, several current research applications, The last three chapters are devoted to the Landau-Wilson approach to critical phenomena. Many new problems and illustrations have been added to this edition. |
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Page 269
... Bose gas . From ( 12.65 ) we see that S = 0 at T 0 , in accordance with the third law of thermodynamics . This means that the condensed phase ( which exists at T ... Bose - Einstein condensation of an ideal Bose gas lies Ideal Bose Gas 269.
... Bose gas . From ( 12.65 ) we see that S = 0 at T 0 , in accordance with the third law of thermodynamics . This means that the condensed phase ( which exists at T ... Bose - Einstein condensation of an ideal Bose gas lies Ideal Bose Gas 269.
Page 273
... gas of phonons . ( b ) Find the velocity of sound in liquid He1 at low temperature . 12.2 . Equation ( 12.64 ) states that G = 0 for v < ve . Using the formula − ( ƏG / ǝT ) ... GASES AT LOW TEMPERATURES 13.1 DEFINITION OF Ideal Bose Gas 273.
... gas of phonons . ( b ) Find the velocity of sound in liquid He1 at low temperature . 12.2 . Equation ( 12.64 ) states that G = 0 for v < ve . Using the formula − ( ƏG / ǝT ) ... GASES AT LOW TEMPERATURES 13.1 DEFINITION OF Ideal Bose Gas 273.
Page 409
Kerson Huang. chapter 19 HARD - SPHERE BOSE GAS 19.1 STATEMENT OF THE PROBLEM A hard - sphere Bose gas is a collection of N spinless bosons , each of mass m , contained in a box of volume V , with the boundary condition that the wave ...
Kerson Huang. chapter 19 HARD - SPHERE BOSE GAS 19.1 STATEMENT OF THE PROBLEM A hard - sphere Bose gas is a collection of N spinless bosons , each of mass m , contained in a box of volume V , with the boundary condition that the wave ...
Contents
THE LAWS OF THERMODYNAMICS | 3 |
SOME APPLICATIONS OF THERMODYNAMICS | 33 |
THE PROBLEM OF KINETIC THEORY | 55 |
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absolute zero approximation assume assumption atoms average becomes Boltzmann Bose calculate called canonical ensemble classical collision complete condition consider constant contains coordinates corresponds defined definition denoted density depends derivation determined discussion distribution effect eigenvalues elements energy ensemble entropy equal equation equilibrium excited exists expansion external fact Fermi field finite given ground Hamiltonian heat Hence ideal independent integral interaction lattice levels limit liquid magnetic mass matrix mean molecular molecules momentum n₁ obtain occupation operator particles partition function phase physical positive possible potential pressure probability problem properties quantity quantum quantum mechanics region represented respectively result satisfies shown in Fig solution specific statistical mechanics temperature theorem theory thermodynamic transformation transition unit V₁ V₂ valid volume wave function