NEW DIFFERENTIAL OPERATORS AND DISCRETIZATION METHODS FOR LARGE-EDDY SIMULATION AND REGULARIZATION MODELING
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Xavier Trias, F.
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Tech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, SpainTech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
Xavier Trias, F.
[1
]
Gorobets, Andrey
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Tech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
Keldysh Inst Appl Math, Moscow 125047, RussiaTech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
Gorobets, Andrey
[1
,2
]
David Perez-Segarra, C.
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Tech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, SpainTech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
David Perez-Segarra, C.
[1
]
Oliva, Assensi
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Tech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, SpainTech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
Oliva, Assensi
[1
]
机构:
[1] Tech Univ Catalonia, Heat & Mass Transfer Technol Ctr, ETSEIAT, C Colom 11, Terrassa 08222, Spain
[2] Keldysh Inst Appl Math, Moscow 125047, Russia
来源:
11TH WORLD CONGRESS ON COMPUTATIONAL MECHANICS; 5TH EUROPEAN CONFERENCE ON COMPUTATIONAL MECHANICS; 6TH EUROPEAN CONFERENCE ON COMPUTATIONAL FLUID DYNAMICS, VOLS V - VI
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2014年
Direct numerical simulations (DNS) of the incompressible Navier-Stokes equations are limited to relatively low-Reynolds numbers. Therefore, dynamically less complex mathematical formulations are necessary for coarse-grain simulations. Regularization and eddy-viscosity models for Large-Eddy Simulation are examples thereof. They rely on differential operators that should be able to capture well different flow configurations (laminar and 2D flows, near-wall behavior, transitional regime. . .). Most of them are based on the combination of invariants of a symmetric second-order tensor that is derived from the gradient of the resolved velocity field. In the present work, they are presented in a framework where all the models are represented as a combination of elements of a 5D phase space of invariants. In this way, new models can be constructed by imposing appropriate restrictions in this space. Moreover, since the discretization errors may play an important role, a novel approach to discretize the viscous term with spatially varying eddy-viscosity is used. It is based on basic operators; therefore, the implementation is straightforward even for staggered formulations. The performance of the proposed methods will be assessed by means of direct comparison to DNS reference results.
机构:
Univ Calif Los Angeles, Joint Inst Reg Earth Syst Sci & Engn, Los Angeles, CA 90095 USA
CALTECH, Jet Prop Lab, Pasadena, CA USA
Univ Lisbon, Inst Dom Luiz, Fac Ciencias, Lisbon, PortugalUniv Calif Los Angeles, Joint Inst Reg Earth Syst Sci & Engn, Los Angeles, CA 90095 USA
Chinita, Maria J.
Matheou, Georgios
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Univ Connecticut, Dept Mech Engn, Storrs, CT USAUniv Calif Los Angeles, Joint Inst Reg Earth Syst Sci & Engn, Los Angeles, CA 90095 USA
Matheou, Georgios
Miranda, Pedro M. A.
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Univ Lisbon, Inst Dom Luiz, Fac Ciencias, Lisbon, PortugalUniv Calif Los Angeles, Joint Inst Reg Earth Syst Sci & Engn, Los Angeles, CA 90095 USA