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 293
... denote the two phases . The symbol a - b signifies that this part of the plane contains the projections of the two phases and those of states where these two phases are present in equilibrium . The symbol ab denotes the single phase ...
... denote the two phases . The symbol a - b signifies that this part of the plane contains the projections of the two phases and those of states where these two phases are present in equilibrium . The symbol ab denotes the single phase ...
Page 308
... denote only the sum of the coefficients of the gaseous substances in the reaction equation . Finally , the law of mass action is valid also for reactions in weak solutions where the solvent as well as the solutes takes part in the ...
... denote only the sum of the coefficients of the gaseous substances in the reaction equation . Finally , the law of mass action is valid also for reactions in weak solutions where the solvent as well as the solutes takes part in the ...
Page 315
... denote a positron and an electron , and y denotes one or more photons . The chemical potential of the photon gas is zero ( § 63 ) . The condition of equilibrium for pair production is therefore μ ++ = 0 , ( 105.1 ) where μ and μ are the ...
... denote a positron and an electron , and y denotes one or more photons . The chemical potential of the photon gas is zero ( § 63 ) . The condition of equilibrium for pair production is therefore μ ++ = 0 , ( 105.1 ) where μ and μ are the ...
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