Throughout Part I we consider a system of classical point particles as the microscopic model for fluid and gases. Particles are identical and interact through a short range central potential. They may be confined to a container. We have to introduce the dynamical laws governing the time evolution, paying particular attention to the case of hard spheres and to boundary conditions.


Phase Space Hard Sphere Gibbs Measure Thermal Boundary Condition Wall Potential 
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Copyright information

© Springer-Verlag Berlin Heidelberg 1991

Authors and Affiliations

  • Herbert Spohn
    • 1
  1. 1.Theoretische PhysikLudwig-Maximilians-Universität MünchenMünchen 2Fed. Rep. of Germany

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