Statistical Physics, Part 1A lucid presentation of statistical physics and thermodynamics which develops from the general principles to give a large number of applications of the theory. |
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Page 6
... subsystem the macroscopic physical quantities are to a high degree of accuracy equal to their mean values , the ... subsystem with the surrounding parts are those near the surface of the subsystem ; the relative number of such particles ...
... subsystem the macroscopic physical quantities are to a high degree of accuracy equal to their mean values , the ... subsystem with the surrounding parts are those near the surface of the subsystem ; the relative number of such particles ...
Page 7
... subsystem does not affect the probabilities of various states of the other subsystems . Let us consider any two subsystems , and let dp1 ) dq ( 1 ) and dp ( 2 ) dq ( 2 ) be volume elements in their phase spaces . If we regard the two ...
... subsystem does not affect the probabilities of various states of the other subsystems . Let us consider any two subsystems , and let dp1 ) dq ( 1 ) and dp ( 2 ) dq ( 2 ) be volume elements in their phase spaces . If we regard the two ...
Page 9
... subsystem . Instead of considering points representing states of one subsystem at different instants t1 , t2 , ... , we may consider simultaneously , in a formal manner , a very large ( in the limit , infinite ) number of exactly ...
... subsystem . Instead of considering points representing states of one subsystem at different instants t1 , t2 , ... , we may consider simultaneously , in a formal manner , a very large ( in the limit , infinite ) number of exactly ...
Contents
Elementary excitations in a quantum Fermi liquid | 1 |
Interaction of quasiparticles | 2 |
Magnetic susceptibility of a Fermi liquid | 3 |
Copyright | |
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atoms axis body Bravais lattice calculate cell chemical potential classical coefficients components concentration condition constant coordinates correlation function corresponding critical point crystal denote density depends derivative determined electron elements entropy equal equation expansion expression Fermi field fluctuations formula free energy frequency gases Gibbs distribution given gives Hamiltonian Hence ideal gas integral interaction irreducible representations liquid macroscopic magnetic matrix mean square mean value molecule momenta momentum motion N₁ number of particles obtain order parameter P₁ partition function phase transition phonon plane pressure PROBLEM properties Quantum Mechanics reciprocal lattice regarded relation result rotational second kind solid solution solvent space group specific heat statistical substance Substituting subsystem suffix surface symmetry temperature theory thermal thermodynamic potential thermodynamic quantities tion total number transformation transition point vapour variables velocity vibrations volume zero ӘР