2009
DOI: 10.1017/s0022112008004965
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A generalized mean-field model of the natural and high-frequency actuated flow around a high-lift configuration

Abstract: A low-dimensional Galerkin model is proposed for the flow around a high-lift configuration, describing natural vortex shedding, the high-frequency actuated flow with increased lift and transients between both states. The form of the dynamical system has been derived from a generalized mean-field consideration. Steady state and transient URANS (unsteady Reynolds-averaged Navier–Stokes) simulation data are employed to derive the expansion modes and to calibrate the system parameters. The model identifies the mea… Show more

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Cited by 87 publications
(71 citation statements)
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References 43 publications
(58 reference statements)
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“…Lift force and drag force fluctuations are most susceptible to variations of the amplitudes of the first odd and even POD modes, which energetically dominate higher odd and even POD modes, respectively (see e.g. Noack et al 2003;Luchtenburg et al 2009). …”
Section: Lift and Drag Optimized Oids Of Cylinder Wake Flowmentioning
confidence: 99%
“…Lift force and drag force fluctuations are most susceptible to variations of the amplitudes of the first odd and even POD modes, which energetically dominate higher odd and even POD modes, respectively (see e.g. Noack et al 2003;Luchtenburg et al 2009). …”
Section: Lift and Drag Optimized Oids Of Cylinder Wake Flowmentioning
confidence: 99%
“…an extension of POD to data compression of multiple operation points, see [17] for sequential POD or [30] for DPOD. We follow an alternative approach suggested in [20,22] of a canonical reduction with parameter identification. Here, a very small system of nonlinear ODEs is adapted to the computed flows in the actuated and non-actuated case.…”
Section: Model Reductionmentioning
confidence: 99%
“…The filter modes contain significant information gained from the URANS solution by the k-ω-model. Following [20,29], the main idea of the ROM is to set up a small size system of ODEs for (a 1 (t), · · · , a 4 (t)) T that rebuilds the computed fluid flow best under the operating conditions. Similarly to the work of Luchtenburg et al [20], the dynamical system consists of the uniformly oscillating of the unactuated and the actuated coefficient pairs (a 1 , a 2 ) respectively (a 3 , a 4 ), which are coupled through the equations for amplified saturation.…”
Section: Reduced-order Model (Rom)mentioning
confidence: 99%
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