dc.creatorGraham, Jonathan Pietarila
dc.creatorHolm, Darryl D.
dc.creatorMininni, Pablo Daniel
dc.creatorPouquet, Annick
dc.date.accessioned2018-10-09T16:37:42Z
dc.date.accessioned2018-11-06T14:51:33Z
dc.date.available2018-10-09T16:37:42Z
dc.date.available2018-11-06T14:51:33Z
dc.date.created2018-10-09T16:37:42Z
dc.date.issued2008-03
dc.identifierGraham, Jonathan Pietarila; Holm, Darryl D.; Mininni, Pablo Daniel; Pouquet, Annick; Three regularization models of the Navier-Stokes equations; American Institute of Physics; Physics of Fluids; 20; 3; 3-2008; 351071-3510715
dc.identifier1070-6631
dc.identifierhttp://hdl.handle.net/11336/61969
dc.identifierCONICET Digital
dc.identifierCONICET
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1891134
dc.description.abstractWe determine how the differences in the treatment of the subfilter-scale physics affect the properties of the flow for three closely related regularizations of Navier-Stokes. The consequences on the applicability of the regularizations as subgrid-scale (SGS) models are also shown by examining their effects on superfilter-scale properties. Numerical solutions of the Clark-α model are compared to two previously employed regularizations, the Lagrangian-averaged Navier-Stokes α-model (LANS-α) and Leray-α, albeit at significantly higher Reynolds number than previous studies, namely, Re≈3300, Taylor Reynolds number of Re≈790, and to a direct numerical simulation (DNS) of the Navier-Stokes equations. We derive the de Kármán-Howarth equation for both the Clark-α and Leray-α models. We confirm one of two possible scalings resulting from this equation for Clark-α as well as its associated k-1 energy spectrum. At subfilter scales, Clark-α possesses similar total dissipation and characteristic time to reach a statistical turbulent steady state as Navier-Stokes, but exhibits greater intermittency. As a SGS model, Clark-α reproduces the large-scale energy spectrum and intermittency properties of the DNS. For the Leray-α model, increasing the filter width α decreases the nonlinearity and, hence, the effective Reynolds number is substantially decreased. Therefore, even for the smallest value of α studied Leray-α was inadequate as a SGS model. The LANS-α energy spectrum ∼k1, consistent with its so-called "rigid bodies," precludes a reproduction of the large-scale energy spectrum of the DNS at high Re while achieving a large reduction in numerical resolution. We find, however, that this same feature reduces its intermittency compared to Clark-α (which shares a similar de Kármán-Howarth equation). Clark-α is found to be the best approximation for reproducing the total dissipation rate and the energy spectrum at scales larger than α, whereas high-order intermittency properties for larger values of α are best reproduced by LANS-α. © 2008 American Institute of Physics.
dc.languageeng
dc.publisherAmerican Institute of Physics
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/https://dx.doi.org/10.1063/1.2880275
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://aip.scitation.org/doi/full/10.1063/1.2880275
dc.rightshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.rightsinfo:eu-repo/semantics/openAccess
dc.titleThree regularization models of the Navier-Stokes equations
dc.typeArtículos de revistas
dc.typeArtículos de revistas
dc.typeArtículos de revistas


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