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 46
... solution , fill the tube with a sugar solution , and then dip this end of the tube into a beaker of water , we find that the sugar solution rises to a height h above the level of the water , as illustra- ted in Fig . 2.12 . This ...
... solution , fill the tube with a sugar solution , and then dip this end of the tube into a beaker of water , we find that the sugar solution rises to a height h above the level of the water , as illustra- ted in Fig . 2.12 . This ...
Page 49
... solution . Hence P ' = n1RT V ( 2.49 ) It is easy to see that the boiling point of a solution is higher than that of the pure solvent , on account of osmotic pressure . To deduce the change in boiling point , let us first find the ...
... solution . Hence P ' = n1RT V ( 2.49 ) It is easy to see that the boiling point of a solution is higher than that of the pure solvent , on account of osmotic pressure . To deduce the change in boiling point , let us first find the ...
Page 50
... solution and the pure solvent . pressure is by definition equal to the pressure exerted by the column of solution of height h : P ' = pgh ( 2.51 ) where p is the density of the solution . Dividing ( 2.50 ) by ( 2.51 ) we have AP vapor P ...
... solution and the pure solvent . pressure is by definition equal to the pressure exerted by the column of solution of height h : P ' = pgh ( 2.51 ) where p is the density of the solution . Dividing ( 2.50 ) by ( 2.51 ) we have AP vapor P ...
Contents
THE LAWS OF THERMODYNAMICS | 3 |
SOME APPLICATIONS OF THERMODYNAMICS | 33 |
THE PROBLEM OF KINETIC THEORY | 55 |
Copyright | |
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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