TY - GEN
T1 - Experimental and numerical investigation of turbulent boundary layers with strong pressure gradients
AU - Knopp, Tobias
AU - Schanz, Daniel
AU - Novara, Matteo
AU - Lühder, Wieland
AU - Strampe, Laura
AU - Schülein, Erich
AU - Schröder, Andreas
AU - Bross, Matthew
AU - Parikh, Agastya
AU - McLellan, David
AU - Eich, Felix
AU - Kähler, Christian J.
N1 - Funding Information:
The funding by DLR within the DLR internal project VicToria and by the institute DLR Institute of Aerodynamics and Flow Technology is gratefully acknowledged. The experimental studies were funded in parts within the DFG-projects “Analyse turbulenter Grenzschichten mit Druckgradient bei großen Reynoldszahlen mit hochauflösenden Vielkameramessverfahren” (Grant KA 1808/14-1 & SCHR 1165/3-1) and by DFG as part of Priority Programme ’Turbulent Superstructures’ (DFG SPP 1881) (Grant No. SCHR 1165/5-1 and KA 1808/21-1). The assistance of Martin Bitter, Rainer Hain, Sven Scharnowski, Janos Agocs and Reinhard Geisler for the wind tunnel experiment, and the valuable discussions with Andreas Krumbein, Cornelia Grabe, Dieter Schwamborn and Cord-Christian Rossow are gratefully acknowledged. Finally, the authors are very grateful to Michel Stanislas, John Eaton, Philip Schlatter, and to the partners of the International Collaboration on Experimental Turbulence (ICET) and in particular to Sean C. C. Bailey and to Ivan Marusic and for kindly providing the data for the canonical TBL at ZPG. Special thanks are to
Funding Information:
The funding by DLR within the DLR internal project VicToria and by the institute DLR Institute of Aerodynamics and Flow Technology is gratefully acknowledged. The experimental studies were funded in parts within the DFGprojects ?Analyse turbulenter Grenzschichten mit Druckgradient bei gro?en Reynoldszahlen mit hochaufl?senden Vielkameramessverfahren? (Grant KA 1808/14-1 & SCHR 1165/3-1) and by DFG as part of Priority Programme ?Turbulent Superstructures? (DFGSPP 1881) (Grant No. SCHR 1165/5-1 and KA 1808/21-1). The assistance of Martin Bitter, Rainer Hain, Sven Scharnowski, Janos Agocs and Reinhard Geisler for the wind tunnel experiment, and the valuable discussions with Andreas Krumbein, Cornelia Grabe, Dieter Schwamborn and Cord-Christian Rossow are gratefully acknowledged. Finally, the authors are very grateful to Michel Stanislas, John Eaton, Philip Schlatter, and to the partners of the International Collaboration on Experimental Turbulence (ICET) and in particular to Sean C. C. Bailey and to Ivan Marusic and for kindly providing the data for the canonical TBL at ZPG. Special thanks are to Stefan Melber-Wilkending for valuable discussions on wind-tunnels.
Publisher Copyright:
© 2022, American Institute of Aeronautics and Astronautics Inc.. All rights reserved.
PY - 2022
Y1 - 2022
N2 - A detailled investigation of a turbulent boundary-layer flow subjected to a strong adverse pressure gradient (APG) is presented. The main goal is to define a test case for the validation and improvement of RANS-turbulence models from wind-tunnel measurement data collected over the course of multiple measurement campaigns, including volumetric Lagrangian Particle Tracking (LPT) and stereoscopic PIV (SPIV), and oil-film interferometry. The boundary layer at a zero-pressure gradient (ZPG) reference position upstream of the pressure gradient region is found to exhibit a mild deviation from a canonical flow in the sense that the boundary layer thickness and hence the Reynolds number based on the momentum loss thickness Reθ are larger than for a canonical flow. Moreover a mild deviation in skin-friction coefficient and shape factor is found. The experimental data using LPT and SPIV in a spanwise domain around the centerplane show an increase of the boundary layer thickness compared to a canonical flow and a spanwise variability. This can possibly be attributed to the wake flow of the turning vanes upstream of the nozzle and the test-section. For the mean velocity profiles, this leads to a deviation in the law-of-the-wake region compared to canonical flows. The inner region, which is essential for the turbulence modelling and validation, is largely unaffected and agrees well with canonical flows. The Reynolds stresses are also in good agreement with canonical flows. Regarding the ultimate aim to define the computational set-up for RANS simulations, a pragmatic approach is pursued. The inlet length of the test-section is increased to account for the larger boundary layer thickness, corresponding to an adjustment of the virtual origin of the boundary layer. This leads to a good matching with the experimental mean velocity profile and the boundary layer parameters at the ZPG reference position. Downstream, in the pressure gradient region, which is the focus region for the improvement and validation of RANS turbulence models, the deviation between the RANS results and the experimental data is found to be almost insensitive with respect to minor changes in the computational set-up. In the strong APG region, the clearly most important deviation between the numerical predictions and the experimental data is due to the RANS turbulence models used.
AB - A detailled investigation of a turbulent boundary-layer flow subjected to a strong adverse pressure gradient (APG) is presented. The main goal is to define a test case for the validation and improvement of RANS-turbulence models from wind-tunnel measurement data collected over the course of multiple measurement campaigns, including volumetric Lagrangian Particle Tracking (LPT) and stereoscopic PIV (SPIV), and oil-film interferometry. The boundary layer at a zero-pressure gradient (ZPG) reference position upstream of the pressure gradient region is found to exhibit a mild deviation from a canonical flow in the sense that the boundary layer thickness and hence the Reynolds number based on the momentum loss thickness Reθ are larger than for a canonical flow. Moreover a mild deviation in skin-friction coefficient and shape factor is found. The experimental data using LPT and SPIV in a spanwise domain around the centerplane show an increase of the boundary layer thickness compared to a canonical flow and a spanwise variability. This can possibly be attributed to the wake flow of the turning vanes upstream of the nozzle and the test-section. For the mean velocity profiles, this leads to a deviation in the law-of-the-wake region compared to canonical flows. The inner region, which is essential for the turbulence modelling and validation, is largely unaffected and agrees well with canonical flows. The Reynolds stresses are also in good agreement with canonical flows. Regarding the ultimate aim to define the computational set-up for RANS simulations, a pragmatic approach is pursued. The inlet length of the test-section is increased to account for the larger boundary layer thickness, corresponding to an adjustment of the virtual origin of the boundary layer. This leads to a good matching with the experimental mean velocity profile and the boundary layer parameters at the ZPG reference position. Downstream, in the pressure gradient region, which is the focus region for the improvement and validation of RANS turbulence models, the deviation between the RANS results and the experimental data is found to be almost insensitive with respect to minor changes in the computational set-up. In the strong APG region, the clearly most important deviation between the numerical predictions and the experimental data is due to the RANS turbulence models used.
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U2 - 10.2514/6.2022-1035
DO - 10.2514/6.2022-1035
M3 - Conference contribution
AN - SCOPUS:85123345031
SN - 9781624106316
T3 - AIAA Science and Technology Forum and Exposition, AIAA SciTech Forum 2022
BT - AIAA SciTech Forum 2022
PB - American Institute of Aeronautics and Astronautics Inc, AIAA
T2 - AIAA Science and Technology Forum and Exposition, AIAA SciTech Forum 2022
Y2 - 3 January 2022 through 7 January 2022
ER -