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 260
... curves must touch . Of the points lying on the curve AKB itself , only the critical point K corresponds to an actually existing state of the homogeneous body ; this is the only point where the curve reaches the region of stable ...
... curves must touch . Of the points lying on the curve AKB itself , only the critical point K corresponds to an actually existing state of the homogeneous body ; this is the only point where the curve reaches the region of stable ...
Page 290
... curves . Let us consider the points on an equilibrium curve at which the concen- tration becomes equal in the two phases . Two cases are possible : ( 1 ) at such a point all other properties of the two phases also become equal , i.e. ...
... curves . Let us consider the points on an equilibrium curve at which the concen- tration becomes equal in the two phases . Two cases are possible : ( 1 ) at such a point all other properties of the two phases also become equal , i.e. ...
Page 294
... curve has no break at the maximum , as in Fig . 21 . Similarly , near a triple point the equilibrium curves have the form shown in Fig . 30. The phase which is a chemical compound is represented by a ver- tical line , to which region II ...
... curve has no break at the maximum , as in Fig . 21 . Similarly , near a triple point the equilibrium curves have the form shown in Fig . 30. The phase which is a chemical compound is represented by a ver- tical line , to which region II ...
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