三维超声速混合层内标量混合的大涡模拟

孙明波; 范晓樯; 梁剑寒; 王振国

三维超声速混合层内标量混合的大涡模拟

国防科技大学航天与材料工程学院, 长沙 410073

基金项目: 国家自然科学基金(90505009)

计量
- 文章访问数: 1931
- HTML浏览量: 406
- PDF量: 442
- 被引次数: 0
出版历程
- 收稿日期: 2006-09-12
- 修回日期: 2006-12-18
- 刊出日期: 2007-09-28

Large eddy simulation of scalar mixing in a 3D supersonic mixing layer

College of Aerospace and Material Engineering, National University of Defense Technology, Changsha 410073, China

摘要

摘要: 对三维对流马赫数0.62的超声速混合层流动的标量混合进行大涡模拟, 控制方程对流项采用五阶精度的WENO格式求解, 小尺度涡的作用采用一方程LDKM亚格子模型处理, 过滤后的组分方程中的亚格子组分对流通量采用梯度扩散模化.模拟得到了混合层流场大尺度拟序结构以及标量场的演化过程, 研究表明标量混合过程受混合层内涡系演化所控制, 标量场具有明显的三维特征.模拟得到的速度、组分及其脉动的统计时均结果和实验结果相符较好.
- 航空、航天推进系统 /
- 超声速混合层 /
- 标量混合 /
- 大涡模拟 /
- 当地动力亚格子动能模型(LDKM)
Abstract: Large eddy simulation was conducted to study the scalar mixing of a 3D supersonic shear layer with convective Mach number 0.62.Governing equations of large scale eddy were solved with fifth-order WENO scheme,and effect of small scale eddy was simulated by using localized dynamic kinetic subgrid scale model(LDKM).The subgrid convective species flux in the filtered species equation was modeled using gradient diffusion method.The results reveal the evolution of the vortex structure of the mixing layer and the scalar field.Simulations show that coherent structures dominate the scalar mixing and the instantaneous distribution of scalar field exhibits obvious 3D characteristics.Statistics such as mean and the root mean square(RMS)of the velocity and the scalar field compares well with the experimental measurements.
- aerospace propulsion system /
- supersonic shear layer /
- scalar mixing /
- large eddy simulation /
- localized dynamic kinetic subgrid scale model(LDKM)

HTML

参考文献(9)

[1]	Clemens N T,Mungal M G.Large scale structure and entrainment in the supersonic mixing layer[J].Journal of Fluid Mechanics[J],1995,284:171-216.
[2]	Sankaran V,Genin F,Menon S.A sub-grid mixing model for large eddy simulation of supersonic combustion[R].AIAA 2004-0801.
[3]	Menon S,Fryxell B.Simulations of strong shock-shear layer interactions in complex domains[R].CCL Report 2004-015,Computational Combustion Laboratory,Georgia Institute of Technology,2004.
[4]	Menon S,Yeung P K,Kim W W.Effect of subgrid models on the computed interscale energy transfer in isotropic turbulence[J].Computers and Fluids,1996,25(2):165-180.
[5]	Blin L,Hadjadj A,Vervisch L.Large eddy simulations of compressible turbulent flows[R].AIAA 99-0787.
[6]	Shu C W.High order ENO and WENO schemes for computational fluid dynamics,in high-order methods for computational physics[M]∥Barth T J,Deconinck H.Lecture notes in computational science and engineering.Volume 9.[S.l]:Springer-Verlage,1999:439-582.
[7]	Poinsot T,Lele S.Boundary conditions for direct simulations of compressible viscous flow[J].Journal of Computational Physics,1992,101(2):104-129.
[8]	Georgiadis N J.Alexander J I D,Reshotko E.Hybrid Reynolds-averaged Navier-Stokes/large-eddy simualtions of supersonic turbulent mixing[J].AIAA Journal,2003,41(2):218-229.
[9]	Sankaran V,Menon S.LES of scalar mixing in supersonic shear layers[J].Proceedings of the combustion Institute,2004,30(2):2835-2842.