Use of eddy viscosity in resolvent analysis of turbulent channel flow

被引:18
|
作者
Symon, Sean [1 ]
Madhusudanan, Anagha [2 ]
Illingworth, Simon J. [3 ]
Marusic, Ivan [3 ]
机构
[1] Univ Southampton, Fac Engn & Phys Sci, Aerodynam & Flight Mech, Southampton SO17 1BJ, England
[2] Univ Cambridge, Ctr Math Sci, Dept Appl Math & Theoret Phys, Cambridge CB3 0WA, England
[3] Univ Melbourne, Dept Mech Engn, Parkville, Vic 3010, Australia
关键词
LARGE-SCALE STRUCTURES; ENERGY AMPLIFICATION; STABILITY;
D O I
10.1103/PhysRevFluids.8.064601
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The predictions obtained from resolvent analysis with and without an eddy viscosity model for turbulent channel flow at Re tau = 550 are compared to direct numerical simulation data to identify the scales and wave speeds for which resolvent analysis provides good predictions. The low-rank behavior of the standard resolvent identifies energetic regions of the flow whereas the eddy resolvent is low rank when the resulting projection of the leading eddy resolvent mode onto the leading mode from spectral proper orthogonal decomposition is maximum. The highest projections are obtained for structures that are associated with the near-wall cycle and structures that are energetic at z = +/- 0.5. It is argued that these types of structures are likely to be correctly predicted for any friction Reynolds number due to the inner and outer scaling of the Cess eddy viscosity profile. The eddy resolvent also correctly identifies the most energetic wave speed for these two scales. For all other scales, neither analysis reliably predicts the most energetic wave speed or mode shapes. The standard resolvent tends to overestimate the most energetic wave speed while the eddy resolvent underestimates it. The resulting eddy resolvent modes are overly "attached" to the wall since the wall-normal gradient of the eddy viscosity overestimates the transport of energy towards the wall. These observations have direct implications for future work towards estimating turbulent channel flows using resolvent analysis and suggest that the Cess profile can be further optimized for individual scales to provide better low-order models of turbulent channel flows.
引用
收藏
页数:26
相关论文
共 50 条
  • [1] Optimisation and modelling of eddy viscosity in the resolvent analysis of turbulent channel flows
    Ying, Anjia
    Chen, Xianliang
    Li, Zhigang
    Fu, Lin
    JOURNAL OF FLUID MECHANICS, 2024, 1001
  • [2] On the role of eddy viscosity in resolvent analysis of turbulent jets
    von Saldern, Jakob G. R.
    Schmidt, Oliver T.
    Jordan, Peter
    Oberleithner, Kilian
    JOURNAL OF FLUID MECHANICS, 2024, 1000
  • [3] Resolvent Analysis for Turbulent Channel Flow with Riblets
    Chavarin, Andrew
    Luhar, Mitul
    AIAA JOURNAL, 2020, 58 (02) : 589 - 599
  • [4] Eddy-viscosity-improved resolvent analysis of compressible turbulent boundary layers
    Fan, Yitong
    Kozul, Melissa
    Li, Weipeng
    Sandberg, Richard D.
    JOURNAL OF FLUID MECHANICS, 2024, 983
  • [5] SIMPLE EDDY VISCOSITY MODEL FOR TURBULENT PIPE AND CHANNEL FLOW
    MEI, J
    SQUIRE, W
    AIAA JOURNAL, 1972, 10 (03) : 350 - &
  • [6] The nature of a universal subgrid eddy viscosity model in a turbulent channel flow
    Gu, Zhaolin
    Jiao, Jianying
    Zhang, Yunwei
    Su, Junwei
    EPL, 2011, 94 (03)
  • [7] ON EDDY VISCOSITY OF INCOMPRESSIBLE TURBULENT FLOW
    STANISIC, MM
    GROVES, RN
    ZEITSCHRIFT FUR ANGEWANDTE MATHEMATIK UND PHYSIK, 1965, 16 (05): : 709 - &
  • [8] Adjoint-based computation of nonlocal eddy viscosity in turbulent channel flow
    Liu, Jessie
    Bryngelson, Spencer H.
    Zaki, Tamer A.
    Mani, Ali
    PHYSICAL REVIEW FLUIDS, 2024, 9 (09):
  • [9] Direct calculation of the eddy viscosity operator in turbulent channel flow at Reτ=180
    Park, Danah
    Mani, Ali
    JOURNAL OF FLUID MECHANICS, 2024, 998
  • [10] A new dynamic subgrid eddy viscosity model with application to turbulent channel flow
    Cui, GX
    Zhou, HB
    Zhang, ZS
    Shao, L
    PHYSICS OF FLUIDS, 2004, 16 (08) : 2835 - 2842