Spatial evolution of wall-imposed disturbance in pipe flow

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Spatial evolution of wall-imposed disturbance in pipe flow Cas van Doorne, 1 Jerry Westerweel, 1 Frans Nieuwstadt (†), Tobias Schneider 2 & Bruno Eckhardt 2 1 Laboratory for Aero & Hydrodynamics, Delft University of Technology The Netherlands 2 Fachbereich Physik, University of Marburg, Germany

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Spatial evolution of wall-imposed disturbance in pipe flow. Cas van Doorne, 1 Jerry Westerweel, 1 Frans Nieuwstadt ( †) , Tobias Schneider 2 & Bruno Eckhardt 2 1 Laboratory for Aero & Hydrodynamics, Delft University of Technology The Netherlands - PowerPoint PPT Presentation

Transcript of Spatial evolution of wall-imposed disturbance in pipe flow

Page 1: Spatial evolution of wall-imposed disturbance in pipe flow

Spatial evolution of wall-imposed disturbance in pipe flow

Cas van Doorne,1 Jerry Westerweel,1 Frans Nieuwstadt (†), Tobias Schneider2 & Bruno Eckhardt2

1Laboratory for Aero & Hydrodynamics, Delft University of TechnologyThe Netherlands2Fachbereich Physik, University of Marburg, Germany

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Motivation

• Transition in pipe flow has remained an unresolved problem (Reynolds 1883)

• Experimental validation of the transition scenario (e.g., DNS by Ma Bing et al. 1999)

• What is the nature of the boundary between laminar and turbulent flow? (Edge of Chaos, Skufka et al. 2006)

• Turbulence control?

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Laminar disturbance mechanism

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Stereo PIV: optical configuration

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Stereo PIV

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The edge of chaos

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Numerical edge trajectory

Skufka, Yorke, Eckhardt, PRL 96 (2006) 174101

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Edge state structure: off-center jet

Experiment Numerical simulation

Re = 2875Re = 3000

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LIF visualization

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z / D = 3.0

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z / D = 5.0

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z / D = 8.1

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z / D = 11.3

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z / D = 14.4

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Fully developed turbulence

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Reconstructed vorticity

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Spectral mode decomposition

DNS S-PIV

Re = 3000, 0.25 Hz

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Conclusions

• Flow transition induced by laminar disturbance mechanism

• High-precision S-PIV set-up for measuring cross-flow• Disturbance mimics the edge of chaos flow structure • Quantitative measurement of development of

streaks into packets of hairpin vortices

• Next: add second disturbance mechanism to achieve flow control in experimental configuration