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 72
... chemical potential of a body ( consisting of identical particles ) is just its thermodynamic potential per molecule . When expressed as a function of P and T , the chemical potential is independent of N. Thus we can imme- diately write ...
... chemical potential of a body ( consisting of identical particles ) is just its thermodynamic potential per molecule . When expressed as a function of P and T , the chemical potential is independent of N. Thus we can imme- diately write ...
Page 264
... chemical potentials must therefore be homogeneous functions of zero order in ... potential 2 we now have = = Νμ . Ω = F- ΣμιΝ ( 85.2 ) and hence again -PV ... chemical potential of each component to be constant throughout the system : μ ...
... chemical potentials must therefore be homogeneous functions of zero order in ... potential 2 we now have = = Νμ . Ω = F- ΣμιΝ ( 85.2 ) and hence again -PV ... chemical potential of each component to be constant throughout the system : μ ...
Page 529
... chemical potential of the substance forming it tends to μ ,, the chemical potential of the liquid in bulk . We shall measure the value of μ ' ( for given P and T ) from this limiting value , i.e. write μ ' + u , in place of μ ' ; thus ...
... chemical potential of the substance forming it tends to μ ,, the chemical potential of the liquid in bulk . We shall measure the value of μ ' ( for given P and T ) from this limiting value , i.e. write μ ' + u , in place of μ ' ; thus ...
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