A derivation of the Liouville equation for hard particle dynamics with non-conservative interactions
T.D. Hurst, B.D. Goddard, M. Wilkinson

TL;DR
This paper derives a modified Liouville equation for systems of particles with non-conservative, instantaneous interactions, addressing challenges in modeling such dynamics accurately.
Contribution
It introduces a weak formulation of the Liouville equation that accounts for non-conservative and instantaneous particle interactions.
Findings
Derived a weak formulation suitable for non-conservative interactions
Addressed exclusion of non-physical particle positions during collisions
Provided an example illustrating the formulation
Abstract
The Liouville equation is of fundamental importance in the derivation of continuum models for physical systems which are approximated by interacting particles. However, when particles undergo instantaneous interactions such as collisions, the derivation of the Liouville equation must be adapted to exclude non-physical particle positions, and include the effect of instantaneous interactions. We present the weak formulation of the Liouville equation for interacting particles with general particle dynamics and interactions, and discuss the results using an example.
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Taxonomy
TopicsGas Dynamics and Kinetic Theory · Theoretical and Computational Physics · Quantum Electrodynamics and Casimir Effect
