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 34
Lev Davidovich Landau, Evgeniĭ Mikhaĭlovich Lifshit︠s︡, Lev Petrovich Pitaevskiĭ. CHAPTER II THERMODYNAMIC QUANTITIES § 9. Temperature Thermodynamic physical quantities are those which describe macroscopic states of bodies . They ...
Lev Davidovich Landau, Evgeniĭ Mikhaĭlovich Lifshit︠s︡, Lev Petrovich Pitaevskiĭ. CHAPTER II THERMODYNAMIC QUANTITIES § 9. Temperature Thermodynamic physical quantities are those which describe macroscopic states of bodies . They ...
Page 70
... thermodynamic potential = W - TS we have dT . = Wo + C , ¿ T - T [ C , ŒT - T√ & & . ( 23.7 ) § 24. The dependence of the thermodynamic quantities on the number of particles As well as the energy and entropy , such thermodynamic quantities ...
... thermodynamic potential = W - TS we have dT . = Wo + C , ¿ T - T [ C , ŒT - T√ & & . ( 23.7 ) § 24. The dependence of the thermodynamic quantities on the number of particles As well as the energy and entropy , such thermodynamic quantities ...
Page 343
... thermodynamic quantities consid- ered above but also by the momentum P of its macroscopic motion relative to the medium . In a state of equilibrium there is no macroscopic motion , i.e. P = 0. Motion may ... Thermodynamic Quantities 343.
... thermodynamic quantities consid- ered above but also by the momentum P of its macroscopic motion relative to the medium . In a state of equilibrium there is no macroscopic motion , i.e. P = 0. Motion may ... Thermodynamic Quantities 343.
Contents
Elementary excitations in a quantum Fermi liquid | 1 |
Interaction of quasiparticles | 2 |
Magnetic susceptibility of a Fermi liquid | 3 |
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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