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 275
... pseudopotentials . 13.2 METHOD OF PSEUDOPOTENTIALS IN TWO - BODY PROBLEMS We consider a system of two particles interacting through a finite - ranged potential which has no bound state . The object of the method of pseudo- potentials is ...
... pseudopotentials . 13.2 METHOD OF PSEUDOPOTENTIALS IN TWO - BODY PROBLEMS We consider a system of two particles interacting through a finite - ranged potential which has no bound state . The object of the method of pseudo- potentials is ...
Page 276
... pseudopotentials is to replace the hard - sphere boundary condition by an inhomogeneous term for the wave equation . Such an idea is familiar in electrostatics , where to find the electrostatic potential in the presence of a metallic ...
... pseudopotentials is to replace the hard - sphere boundary condition by an inhomogeneous term for the wave equation . Such an idea is familiar in electrostatics , where to find the electrostatic potential in the presence of a metallic ...
Page 416
... pseudo- potentials . This is actually not so . In every term of the series appearing in ( 19.32 ) , N is raised to ... pseudopotentials can contribute only to what is designated as “ remainder " in ( 19.32 ) . Therefore we can continue ...
... pseudo- potentials . This is actually not so . In every term of the series appearing in ( 19.32 ) , N is raised to ... pseudopotentials can contribute only to what is designated as “ remainder " in ( 19.32 ) . Therefore we can continue ...
Contents
THE LAWS OF THERMODYNAMICS | 3 |
SOME APPLICATIONS OF THERMODYNAMICS | 33 |
4 | 46 |
Copyright | |
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absolute zero approximation atoms average Boltzmann transport equation Bose gas bosons boundary condition calculate classical collision consider constant coordinates corresponds d³r d³v defined denoted density derivation distribution function E₁ eigenvalues energy levels entropy equilibrium excited Fermi gas fermions finite given grand canonical ensemble Hamiltonian hard-sphere Helmholtz free energy Hence ideal Bose gas ideal gas independent integral interaction Ising model isotherm lattice law of thermodynamics liquid He¹ log 2(z macroscopic magnetic matrix elements Maxwell-Boltzmann distribution microcanonical ensemble molecular chaos molecules momentum N₁ N₂ number of particles obtain occupation numbers P₁ partition function phase transition phonons potential pressure pseudopotentials r₁ second law shown in Fig sinh solution specific heat spin statistical mechanics superfluid T-space T₁ temperature theorem transformation V₁ V₂ valid vector velocity volume wave function ди др