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 266
... tion , and from the above hypothesis c <<< 1 . = Let us derive an expression for the thermodynamic potential of the solu- tion . Let Ø 。( P , T , N ) be the thermodynamic potential of the pure solvent ( containing no solute ) ...
... tion , and from the above hypothesis c <<< 1 . = Let us derive an expression for the thermodynamic potential of the solu- tion . Let Ø 。( P , T , N ) be the thermodynamic potential of the pure solvent ( containing no solute ) ...
Page 524
... tion of the corresponding solution . The number no thus defined may be either greater or less than the actual total number n of solute particles . If n1 = n - no > 0 , this means that the solute accumulates at a higher concentra- tion ...
... tion of the corresponding solution . The number no thus defined may be either greater or less than the actual total number n of solute particles . If n1 = n - no > 0 , this means that the solute accumulates at a higher concentra- tion ...
Page 534
... tion producing a nucleus is proportional to exp ( − Rmin / T ) , where Rmin is the minimum work needed to form the nucleus . Since the temperature and chem- ical potential of the nucleus have the same values as in the surrounding ...
... tion producing a nucleus is proportional to exp ( − Rmin / T ) , where Rmin is the minimum work needed to form the nucleus . Since the temperature and chem- ical potential of the nucleus have the same values as in the surrounding ...
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