2005
DOI: 10.1007/s10494-005-4136-0
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Experimental 3D Analysis of the Large Scale Behaviour of a Plane Turbulent Mixing Layer

Abstract: A new structure education method is proposed for representing the three dimensional large scale structures from hot wires measurement data. Due to the limited number of hot wire probes that can be used simultaneously, we firstly have to optimise the spatial location of sensors in order to detect large scale coherent structures. For such a purpose a detailed analysis of the 3D space-time flow organisation is given with particular emphasis on the full two point correlation tensor of the velocity field. Secondly,… Show more

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Cited by 26 publications
(9 citation statements)
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“…Using this property, POD has been also intensively used to formulate a low order dynamical system (Holmes et al, 1996). Furthermore, POD procedure can be also used as an advanced mathematical tool for the reconstruction of missing experimental data, not only in the space domain (Druault and Delville, 2000;Druault et al, 2005a;Druault and Chaillou, 2007) but also in the temporal domain (Druault et al, 2005b). After recalling the mathematical concept of the POD, its application from 2D PIV database is presented.…”
Section: Proper Orthogonal Decomposition (Pod) Mathematical Toolmentioning
confidence: 99%
“…Using this property, POD has been also intensively used to formulate a low order dynamical system (Holmes et al, 1996). Furthermore, POD procedure can be also used as an advanced mathematical tool for the reconstruction of missing experimental data, not only in the space domain (Druault and Delville, 2000;Druault et al, 2005a;Druault and Chaillou, 2007) but also in the temporal domain (Druault et al, 2005b). After recalling the mathematical concept of the POD, its application from 2D PIV database is presented.…”
Section: Proper Orthogonal Decomposition (Pod) Mathematical Toolmentioning
confidence: 99%
“…The latter employed an unconditional estimate of the raw velocity field in a two-dimensional subsonic mixing layer via linear stochastic estimation (LSE), followed by a low-dimensional description of the model estimate via POD. Since then, the joint implementation of these analysis tools (POD and LSE) have taken many different forms in the experimental community using a variety of different flows (backward facing ramps (Taylor & Glauser 2004), axisymmetric sudden expansions (Tinney et al 2002), axisymmetric backward facing steps (Hudy, Naguib & Humphreys 2007) plane mixing layers (Druault, Delville & Bonnet 2005), cavity flows (Murray & Ukeiley 2006), axisymmetric jet flows (Ewing & Citriniti 1999;Picard & Delville 2000;Taylor, Ukeiley & Glauser 2001;Tinney et al 2005Tinney et al , 2006Iqbal & Thomas 2007), pressure fields in the periphery of axisymmetric jets (Coiffet et al 2004), wall jets (Hall & Ewing 2006) and incipiently separated airfoils (Glauser et al 2004;Pinier et al 2007)).…”
Section: Introductionmentioning
confidence: 99%
“…Several structure eduction methodologies based on different flow structure concepts are now well established. For instance, the decomposition of experimental or numerical turbulent flow data can be performed from phase averaging methods or turbulence filterings [2,3], wavelet decomposition [4], stochastic estimation [5,6], proper orthogonal decomposition (POD) [7], etc. But these methods are generally used to characterize only the coherent part of the flow field.…”
Section: Introductionmentioning
confidence: 99%