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2010
Consider a monatomic gas with N molecules enclosed in a recipient of volume V. One molecule of this gas can be specified at a given time by its position x = (x1,x2,x3) and velocity c = (c1,c2,c3). Hence, a molecule can be specified as a point in a six-dimensional space spanned by its coordinates and velocity components, the so-called μ-phase space.
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Consider a monatomic gas with N molecules enclosed in a recipient of volume V. One molecule of this gas can be specified at a given time by its position x = (x1,x2,x3) and velocity c = (c1,c2,c3). Hence, a molecule can be specified as a point in a six-dimensional space spanned by its coordinates and velocity components, the so-called μ-phase space.
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1994
We present a global existence result of weak solutions for Boltzmann equation obtained by R.J. DiPerna and the author. This result is based upon convergence properties of solutions of Boltzmann equation that we recall and discuss.
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We present a global existence result of weak solutions for Boltzmann equation obtained by R.J. DiPerna and the author. This result is based upon convergence properties of solutions of Boltzmann equation that we recall and discuss.
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The Poisson–Boltzmann equation and its application to polyelectrolytes
Journal of Chemical Physics, 1979Fixman Marshall
exaly
A novel lattice Boltzmann model for the Poisson equation
Applied Mathematical Modelling, 2008Zhenhua Chai, Baochang Shi
exaly