Transient growth analysis of the flow past a circular cylinder

被引:38
作者
Abdessemed, N. [1 ]
Sharma, A. S. [1 ,2 ]
Sherwin, S. J. [1 ]
Theofilis, V. [3 ]
机构
[1] Univ London Imperial Coll Sci Technol & Med, Dept Aeronaut, London SW7 2AZ, England
[2] Univ London Imperial Coll Sci Technol & Med, Dept Elect & Elect Engn, London SW7 2AZ, England
[3] Univ Politecn Madrid, Sch Aeronaut, E-28040 Madrid, Spain
基金
英国工程与自然科学研究理事会;
关键词
bifurcation; convection; external flows; flow instability; Navier-Stokes equations; pulsatile flow; shapes (structures); singular value decomposition; CONVECTIVE INSTABILITY; LINEAR-STABILITY; FINITE-ELEMENT; BOUNDARY-LAYER; 3-DIMENSIONAL INSTABILITY; OPTIMAL PERTURBATIONS; TRANSITION; ABSOLUTE; STEADY; MODES;
D O I
10.1063/1.3112738
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
We apply direct transient growth analysis in complex geometries to investigate its role in the primary and secondary bifurcation/transition process of the flow past a circular cylinder. The methodology is based on the singular value decomposition of the Navier-Stokes evolution operator linearized about a two-dimensional steady or periodic state which leads to the optimal growth modes. Linearly stable and unstable steady flow at Re=45 and 50 is considered first, where the analysis demonstrates that strong two-dimensional transient growth is observed with energy amplifications of order of 10(3) at U-infinity tau/D approximate to 30. Transient growth at Re=50 promotes the linear instability which ultimately saturates into the well known von-Kaacutermaacuten street. Subsequently we consider the transient growth upon the time-periodic base state corresponding to the von-Kaacutermaacuten street at Re=200 and 300. Depending upon the spanwise wavenumber the flow at these Reynolds numbers are linearly unstable due to the so-called mode A and B instabilities. Once again energy amplifications of order of 10(3) are observed over a time interval of tau/T=2, where T is the time period of the base flow shedding. In all cases the maximum energy of the optimal initial conditions are located within a diameter of the cylinder in contrast to the spatial distribution of the unstable eigenmodes which extend far into the downstream wake. It is therefore reasonable to consider the analysis as presenting an accelerator to the existing modal mechanism. The rapid amplification of the optimal growth modes highlights their importance in the transition process for flow past circular cylinder, particularly when comparing with experimental results where these types of convective instability mechanisms are likely to be activated. The spatial localization, close to the cylinder, of the optimal initial condition may be significant when considering strategies to promote or control shedding.
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页数:13
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