Abstract
At the Advanced NATO Study Institute at Zwiesel in 1979 I gave a few lectures on the atomic theory of liquid dynamics. The theory was based on the Zwanzig-Mori memory function approach. Since then the whole field has matured and we have seen some more applications of the theory. However, the conceptual ideas have not changed and I will here repeat several points, which I stressed at that time. This kind of theory can be viewed as a generalization both of the ordinary Boltzmann equation for dilute gases and of the Vlasov equation for classical plasmas. For both of them one introduces the density in the six-dimensional phase space, denoted by f\( (\vec{r}\vec{p}t) \). Its evolution in time is in the appropriate situations governed by these equations. The linearized version of the Vlasov equation reads
, where v(r) is the interparticle (Coulomb) potential, m is the particle mass, and \( {f^{{eq}}}(p) = n{\phi_M}(p) \) is the equilibrium distribution, with n being the uniform particle density and 4>M(p) the normalized Maxwellian momentum distribution. The linearized Boltzmann equation takes the form
with a kernel \( K(\vec{p},\vec{p}') \), which contains information on the effect of a single binary collision. The interaction between the particles enters in \( K(\vec{p},\vec{p}') \) through the binary collision cross section.
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© 1987 Martinus Nijhoff Publishers, Dordrecht
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Sjölander, A. (1987). Atomic Motions in Liquids. In: Lüscher, E., Fritsch, G., Jacucci, G. (eds) Amorphous and Liquid Materials. NATO ASI Series, vol 118. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-3505-1_19
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DOI: https://doi.org/10.1007/978-94-009-3505-1_19
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