全部 标题 作者
关键词 摘要

OALib Journal期刊
ISSN: 2333-9721
费用:99美元

查看量下载量

相关文章

更多...

A Note on Taylor-Eddy and Kovasznay Solutions of NS- -Deconvolution and Leray- -Deconvolution Models

DOI: 10.1155/2014/959038

Full-Text   Cite this paper   Add to My Lib

Abstract:

We show that both the Taylor-eddy and Kovasznay exact solutions of the Navier-Stokes equations are also exact solutions of both the NS-α-deconvolution and Leray-α-deconvolution models, but with modified pressures that converge to the Navier-Stokes pressure solution as or the order of deconvolution tends to infinity. The existence of these exact model solutions will provide for better benchmark testing and validation of numerical codes and also shows that the models preserve these special structures. 1. Introduction The Leray- and NS- models and variations thereof have become of significant interest in both the mathematical and engineering communities interested in reduced-order fluid flow modeling. It is the purpose of this paper to derive exact solutions for these models, specifically those of Taylor-eddy and Kovasznay type, both for the purpose of providing better benchmark solutions for computational testing and to show that these models preserve some of the special structures of Navier-Stokes solutions. Solutions of Taylor-eddy type have been shown to exist for the Stolz-Adams approximate deconvolution model by Layton in [1] and for the Rational model by Berselli in [2], thus showing that existence of such solutions for models is important for model comparisons. To our knowledge, no other model has been shown to admit exact Kovasznay solutions. Denoting by overbar the -filter , the models are defined by the following: Leray- NS- In this work, we will consider these models in , or 3. The solutions we develop will satisfy the models pointwise, and so the models could also be equipped with boundary conditions, provided they are consistent with the solutions. The Leray model was developed by Leray in 1934 (but using a Gaussian filter instead of the -filter) as a theoretical tool to better understand the Navier-Stokes equations [3]. The model was then revisited by Cheskidov et al. in [4] with the -filter, and they proved fundamental properties of the model including well-posedness and agreement of the energy spectrum with that of true fluid flow on the large scales and an increased rate on the small scales (thus showing that the model is more computable). Work in [5] proved a microscale for the model, which better quantified its advantage in computability versus the Navier-Stokes equations. All of these properties are also valid for NS- [6, 7], but NS- also has several advantages over Leray- from the theoretical point of view such as helicity conservation [6], frame invariance [8], and adherence to Kelvin’s circulation theorem [6]. Numerous numerical

References

[1]  W. Layton, “On Taylor/Eddy solutions of approximate deconvolution models of turbulence,” Applied Mathematics Letters, vol. 24, no. 1, pp. 23–26, 2011.
[2]  L. Berselli, “On the large eddy simulation of the Taylor-Green vortex,” Journal of Mathematical Fluid Mechanics, vol. 7, pp. S164–S191, 2005.
[3]  J. Leray, “Sur le mouvement d'un liquide visqueux emplissant l'espace,” Acta Mathematica, vol. 63, no. 1, pp. 193–248, 1934.
[4]  A. Cheskidov, D. D. Holm, E. Olson, and E. S. Titi, “On a Leray-α model of turbulence,” Proceedings of the Royal Society A, vol. 461, no. 2055, pp. 629–649, 2005.
[5]  W. Layton, C. C. Manica, M. Neda, and L. G. Rebholz, “The joint helicity-energy cascade for homogeneous isotropic turbulence generated by approximate deconvolution models,” Advances and Applications in Fluid Mechanics, vol. 4, pp. 1–46, 2008.
[6]  C. Foias, D. D. Holm, and E. S. Titi, “The Navier-Stokes-alpha model of fluid turbulence,” Physica D, vol. 152-153, pp. 505–519, 2001.
[7]  C. Foias, D. D. Holm, and E. S. Titi, “The three dimensional viscous Camassa-Holm equations, and their relation to the Navier-Stokes equations and turbulence theory,” Journal of Dynamics and Differential Equations, vol. 14, no. 1, pp. 1–35, 2002.
[8]  J. L. Guermond, J. T. Oden, and S. Prudhomme, “An interpretation of the Navier-Stokes-alpha model as a frame-indifferent Leray regularization,” Physica D, vol. 177, no. 1–4, pp. 23–30, 2003.
[9]  A. L. Bowers, T.-Y. Kim, M. Neda, L. G. Rebholz, and E. Fried, “The Leray-αβ-deconvolution model: energy analysis and numerical algorithms,” Applied Mathematical Modelling, vol. 37, no. 3, pp. 1225–1241, 2013.
[10]  B. J. Geurts and D. D. Holm, “Leray and LANS-α modelling of turbulent mixing,” Journal of Turbulence, vol. 7, no. 10, pp. 1–33, 2006.
[11]  D. Holm and B. T. Nadiga, “Modeling mesoscale turbulence in the barotropic double-gyre circulation,” Journal of Physical Oceanography, vol. 33, pp. 2355–2365, 2003.
[12]  B. J. Geurts and D. D. Holm, “Regularization modeling for large-eddy simulation,” Physics of Fluids, vol. 15, no. 1, pp. L13–L16, 2003.
[13]  J. Pietarila Graham, D. D. Holm, P. Mininni, and A. Pouquet, “The effect of subfilter-scale physics on regularization models,” Journal of Scientific Computing, vol. 49, no. 1, pp. 21–34, 2011.
[14]  W. J. Layton and L. G. Rebholz, “Approximate deconvolution models of turbulence: analysis, phenomenology and numerical analysis,” Lecture Notes in Mathematics, vol. 2042, pp. 1–192, 2012.
[15]  S. Chen, D. D. Holm, L. G. Margolin, and R. Zhang, “Direct numerical simulations of the Navier-Stokes alpha model,” Physica D, vol. 133, no. 1–4, pp. 66–83, 1999.
[16]  S. Chen, C. Foias, D. D. Holm, E. Olson, E. S. Titi, and S. Wynne, “The Camassa-Holm equations and turbulence,” Physica D, vol. 133, no. 1–4, pp. 49–65, 1999.
[17]  S. Stolz and N. A. Adams, “An approximate deconvolution procedure for large-eddy simulation,” Physics of Fluids, vol. 11, no. 7, pp. 1699–1701, 1999.
[18]  S. Stolz, N. A. Adams, and L. Kleiser, “The approximate deconvolution model for large-eddy simulation of compressible flows and its application to shock-turbulent-boundary-layer interaction,” Physics of Fluids, vol. 13, no. 10, pp. 2985–3001, 2001.
[19]  S. Stolz, N. A. Adams, and L. Kleiser, “An approximate deconvolution model for large-eddy simulation with application to incompressible wall-bounded flows,” Physics of Fluids, vol. 13, no. 4, pp. 997–1015, 2001.
[20]  A. Dunca and Y. Epshteyn, “On the stolz-adams deconvolution model for the large-eddy simulation of turbulent flows,” SIAM Journal on Mathematical Analysis, vol. 37, no. 6, pp. 1890–1902, 2006.
[21]  A. J. Chorin, “Numerical solution for the Navier-Stokes equations,” Mathematics of Computation, vol. 22, pp. 745–762, 1968.
[22]  C. R. Ethier and D. A. Steinman, “Exact fully 3D Navier-Stokes solutions for benchmarking,” International Journal for Numerical Methods in Fluids, vol. 19, no. 5, pp. 369–375, 1994.
[23]  L. I. G. Kovasznay, “Laminar ow behind a two-dimensional grid,” Proceedings of the Cambridge Philosophical Society, vol. 44, pp. 58–62, 1947.
[24]  D. D. Holm, V. Putkaradze, P. D. Weidman, and B. A. Wingate, “Boundary effects on exact solutions of the Lagrangian-averaged Navier-Stokes-α equations,” Journal of Statistical Physics, vol. 113, no. 5-6, pp. 841–854, 2003.

Full-Text

comments powered by Disqus

Contact Us

service@oalib.com

QQ:3279437679

WhatsApp +8615387084133

WeChat 1538708413