Hamiltonian hydrodynamic reductions of one-dimensional Vlasov equations
Rayan Oufar, Cristel Chandre
TL;DR
This work presents a unified Hamiltonian framework for reducing the 1D Vlasov-Poisson system to hydrodynamic-like fluid models with an arbitrary number of variables. By exploiting hydrodynamic Poisson brackets and Casimir invariants, the authors identify normal variables in which all known Hamiltonian closures (multi-delta, waterbag, Burby, and Chandre four-field) are polynomial and share a single generating moment, $μ_2$, which is cubic. The closures are transparently described parametrically via a set of normal variables, revealing a structural connection among diverse models and enabling a compact Hamiltonian description of reduced dynamics with preserved Casimir invariants. This structural unification suggests avenues for data-driven or sparsity-based discovery of closure relations while maintaining the Hamiltonian character of the reduced Vlasov-Poisson dynamics.
Abstract
We investigate Hamiltonian fluid reductions of the one-dimensional Vlasov-Poisson equation. Our approach utilizes the hydrodynamic Poisson bracket framework, which allows us to systematically identify fundamental normal variables derived from the analysis of the Casimir invariants of the resulting Poisson bracket. This framework is then applied to analyze several well-established Hamiltonian closures of the onedimensional Vlasov equation, including the multi-delta distribution and the waterbag models. Our key finding is that all of these seemingly distinct closures consistently lead to the formulation of a unified form of parametric closures: When expressed in terms of the identified normal variables, the parameterization across all these closures is revealed to be polynomial and of the same degree. All these parametric closures are uniquely generated from one of the moments, called $μ$2, a cubic polynomial in the normal variables. This result establishes a structural connection between these different physical models, offering a path toward a more unified and simplified description of the one-dimensional Vlasov-Poisson dynamics through its reduced hydrodynamic forms with an arbitrary number of fluid variables.
