2014
DOI: 10.1016/j.na.2014.07.005
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A Hamiltonian vorticity–dilatation formulation of the compressible Euler equations

Abstract: Using the Hodge decomposition on bounded domains the compressible Euler equations of gas dynamics are reformulated using a density weighted vorticity and dilatation as primary variables, together with the entropy and density. This formulation is an extension to compressible flows of the well-known vorticity-stream function formulation of the incompressible Euler equations. The Hamiltonian and associated Poisson bracket for this new formulation of the compressible Euler equations are derived and extensive use i… Show more

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Cited by 11 publications
(7 citation statements)
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“…Beyond this basic class of PH systems (which however covers different linear and nonlinear physical phenomena), there exists a growing number of PH models for different physical phenomena, see e. g. [54] for the modeling of the plasma in a fusion reactor, [21] for the reactive Navier-Stokes flow or [55] for irreversible thermodynamic systems to mention only a few interesting examples. In [56], a PH formulation of the compressible Euler equations in terms of density, weighted vorticity and dilatation is presented. The PH representation is not unique.…”
Section: Examplesmentioning
confidence: 99%
See 1 more Smart Citation
“…Beyond this basic class of PH systems (which however covers different linear and nonlinear physical phenomena), there exists a growing number of PH models for different physical phenomena, see e. g. [54] for the modeling of the plasma in a fusion reactor, [21] for the reactive Navier-Stokes flow or [55] for irreversible thermodynamic systems to mention only a few interesting examples. In [56], a PH formulation of the compressible Euler equations in terms of density, weighted vorticity and dilatation is presented. The PH representation is not unique.…”
Section: Examplesmentioning
confidence: 99%
“…The vectors of discrete flows and efforts f p/q , e p/q that satisfy (56), together with the discrete boundary ports of different causality, define a subset of the bond space…”
Section: Power Balance On the Discrete Bond Spacementioning
confidence: 99%
“…The SDS describing the system is nonlinear; however, it was also shown that for irrotational flow, the underlying SDS becomes the canonical one. An extended model describing the case of non-isentropic fluids is presented in Polner & van der Vegt (2014) in terms of the vorticity-dilatation variables. Moreover, for the spatial one-dimensional case, different pH models of fluid-thermal equations can be found in Lopezlena & Scherpen (2004b), a dpH of Navier-Stokes equations for reactive flows can be found in Altmann & Schulze (2017), while jet-bundle formulations of the Kortweg-de Vries and Boussinesq equations can be found in Maschke & van der Schaft (2013).…”
Section: Fluid Mechanicsmentioning
confidence: 99%
“…The procedure to construct the port-Hamiltonian model we are aiming for relies greatly on understanding the underlying geometric structure of the state space of each energetic subsystem. This geometric formulation, pioneered by [8] and [9], will allow a systematic derivation of the underlying Hamiltonian dynamical equations and Dirac structures, usually postulated a priori in the literature [10,6,11,12]. Furthermore, it will allow for the boundary terms, which are always absent in the traditional Hamiltonian picture, to be easily identified and transformed into power ports which can be used for energy exchange through the boundary of the spatial domain.…”
mentioning
confidence: 99%