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2014
DOI: 10.1016/j.aop.2014.05.011
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Higher-order Hamiltonian fluid reduction of Vlasov equation

Abstract: From the Hamiltonian structure of the Vlasov equation, we build a Hamiltonian model for the first three moments of the Vlasov distribution function, namely, the density, the momentum density and the specific internal energy. We derive the Poisson bracket of this model from the Poisson bracket of the Vlasov equation, and we discuss the associated Casimir invariants.

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Cited by 19 publications
(18 citation statements)
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“…(12) with where R and T are given by Eqs. (28)- (29). The dependence of the functions R and T in their arguments is not trivial.…”
Section: Model Without Normal Variablesmentioning
confidence: 99%
See 1 more Smart Citation
“…(12) with where R and T are given by Eqs. (28)- (29). The dependence of the functions R and T in their arguments is not trivial.…”
Section: Model Without Normal Variablesmentioning
confidence: 99%
“…Inserting this expression into the previous equations provides the necessary constraints a = 0 and ψ(ξ) = ψ 0 . As a consequence, this model does not have Casimir invariants of the entropy-type [29], i.e., of the form ρφ(S 2 , S 3 ) dx. Moreover, we can show in a similar way that Eq.…”
Section: Model Without Normal Variablesmentioning
confidence: 99%
“…Linear closures, on the other hand, are those selected for drift and gyrokinetic models in the "δf approximation " [28,30]. Following this approach also a new Hamiltonian fluid model obtained from the Vlasov equation has been derived [31]. These results, however, concern fluid models retaining only a very low number of moments, more precisely two-moment models for Refs.…”
Section: Introductionmentioning
confidence: 98%
“…It can be also observed in continuum simulations of the Vlasov equation and electromagnetic field, e.g., [9]. The emergence of dissipative phenomena from reversible equations is also observed when proposing closure relations in the Grad hierarchy, e.g., [10][11][12][13].…”
Section: Introductionmentioning
confidence: 83%