Journal of Mathematical Physics · 1967 · 37 citations · 12 references
Natural SciencesMathematicsPhysicsFluid DynamicsTheoretical PhysicsThermodynamicsBoltzmann Transport EquationSecond Law Of ThermodynamicsBoltzmann EquationsDiscrete Velocity ModelsEquilibrium Distribution FunctionsEquilibrium Population DistributionLinearized Boltzmann EquationNonlinear Boltzmann Equation
It has been conjectured by McKean that the particular property of Boltzmann's H function which singles it out from a wide class of functionals of the Boltzmann solution may be that its successive derivatives alternate in sign. We consider here the proof of this alternating property for a discrete velocity gas. For the linearized-model Boltzmann equation, the proof is trivial. For the full (i.e., nonlinear) model Boltzmann equation, the proof is shown to be equivalent to demonstrating the positivity of a particular polynomial. The proof of this property is then demonstrated. It is also shown that H(n), like H(1), is zero only for the equilibrium distribution.
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<i>Probability and Related Topics in Physical Sciences</i>
Mark Kac, G. E. Uhlenbeck, A. R. Hibbs et al. · Physics Today · 1960 · 665 citations
Shock Structure in a Simple Discrete Velocity Gas
James E. Broadwell · The Physics of Fluids · 1964 · 361 citations
<i>The Conceptual Foundations of the Statistical Approach in Mechanics</i>
P. Ehrenfest, Tatiana Ehrenfest, Michael J. Moravcsik et al. · Physics Today · 1960 · 332 citations