INCA - Computational Fluid Dynamics as good as it gets. - Shock Wave / Boundary Layer Interaction

L. Laguarda, S. Hickel (2024)
Physics of Fluids 36: 081708. doi: 10.1063/5.0227332

We revisit the origin of low-frequency unsteadiness in turbulent recirculation bubbles (TRBs), and, in particular, the hypothesis of a dynamic feedback mechanism between unconstrained separation and reattachment locations. Our results demonstrate, for the first time, effective suppression of the low-frequency characteristics of the TRB without reducing its size, strongly supporting our hypothesis.

W. Wu, L. Laguarda, D. Modesti, S. Hickel (2024)
Flow, Turbulence and Combustion (in press) doi: 10.1007/s10494-024-00580-0

A novel passive flow-control method for shock-wave/turbulent boundary-layer interactions (STBLI) is investigated. The method relies on a structured roughness pattern constituted by streamwise-aligned ridges. Its effectiveness is assessed with wall-resolved large-eddy simulations of the interaction of a Mach 2 turbulent boundary layer flow with an oblique impinging shock with shock angle 40°. A parametric study is performed to investigate the effect of the spacing between the ridges. We find that ridges with small spacing effectively mitigate the low-frequency unsteadiness of STBLI and slightly reduce total-pressure loss.

L. Laguarda, S. Hickel, F.F.J. Schrijer, B.W. van Oudheusden (2024)
Journal of Fluid Mechanics 989: A20. doi:10.1017/jfm.2024.361

We investigate Reynolds number effects in strong shock-wave/turbulent-boundary layer interactions (STBLI) by leveraging a new database of wall-resolved and long-integrated large-eddy simulations (LES). The database encompasses STBLI with massive boundary-layer separation at Mach 2.0, impinging-shock angle 40° and friction Reynolds numbers Re_τ= 355, Re_τ= 1226, and Re_τ= 5118.

A.O. Başkaya, S. Hickel, S.D. Dungan, C. Brehm (2024)
AIAA SciTech, NATO AVT-346: Instability and Transition in Hypersonic Separated Flows, Orlando. AIAA paper 2024-0501. doi: 10.2514/6.2024-0501

Direct numerical simulations (DNS) are performed over a 15° compression ramp undergoing ablation at Mach 8 to examine fluid-ablation interactions (FAI) on transitional high-speed boundary layers. The experiments at these conditions with a rigid wall are first numerically replicated for a laminar baseflow. Heating streaks are introduced by adding perturbations in the baseflow informed by prior stability calculations. The ramp is then replaced by a low-temperature ablator in our DNS and the interaction of the streaks with the recessing ablator surface are examined. Different approaches from two independently developed solvers are used to study this problem.

L. Laguarda, S. Hickel, F.F.J. Schrijer, B.W. van Oudheusden (2024)
Physics of Fluids 36: 016120. doi: 10.1063/5.0179082

The dynamic coupling between a Mach 2.0 shock-wave/turbulent boundary-layer interaction (STBLI) and a flexible panel is investigated. Wall-resolved large-eddy simulations are performed for a baseline interaction over a flat-rigid wall, a coupled interaction with a flexible panel, and a third interaction over a rigid surface that is shaped according to the mean panel deflection of the coupled case.

S.E.M. Niessen, K.J. Groot, S. Hickel, V.E. Terrapon (2023)
Physics of Fluids 35: 024101. doi: 10.1063/5.0135590

Linear stability analyses are performed to study the dynamics of linear convective instability mechanisms in a laminar shock-wave/boundary-layer interaction at Mach 1.7. In order to account for all two-dimensional gradients elliptically, we introduce perturbations into an initial-value problem that are found as solutions to an eigenvalue problem formulated in a moving frame of reference.

W. Hu, S. Hickel, B.W. van Oudheusden (2022)
Journal of Fluid Mechanics 949: A2. doi: 10.1017/jfm.2022.737

The flow over a forward-facing step (FFS) at Ma_∞=1.7 and Re_? = 13 718 is investigated by well-resolved large-eddy simulation. To investigate effects of upstream flow structures and turbulence on the low-frequency dynamics of the shock wave/boundary layer interaction (SWBLI), two cases are considered: one with a laminar inflow and one with a turbulent inflow.

L. Laguarda, J. Santiago Patterson, F.F.J. Schrijer, B.W. van Oudheusden, S. Hickel (2021)
Shock Waves 3: 457-468. doi: 10.1007/s00193-021-01029-3

Experiments on shock–shock interactions were conducted in a transonic–supersonic wind tunnel with variable free-stream Mach number functionality. Transition between the regular interaction (RI) and the Mach interaction (MI) was induced by variation of the free-steam Mach number for a fixed interaction geometry, as opposed to most previous studies where the shock generator angles are varied at constant Mach number.

W. Hu, S. Hickel, B.W. van Oudheusden (2021)
Journal of Fluid Mechanics 915: A107. doi: 10.1017/jfm.2021.95

The low-frequency unsteady motions behind a backward-facing step (BFS) in a turbulent flow at Ma=1.7 and Re_∞=1.3718×10⁷ m⁻¹ are investigated using a well-resolved large-eddy simulation.

W. Hu, S. Hickel, B.W. van Oudheusden (2020)
Phys. Fluids 32: 056102. doi: 10.1063/5.0005431

The development of primary and secondary instabilities is investigated numerically for a supersonic transitional flow over a backward-facing step at Ma = 1.7 and Re_δ=13718. Oblique Tollmien–Schlichting (T–S) waves with properties according to linear stability theory (LST) are introduced at the domain inlet with zero, low, or high amplitude (cases ZA, LA, and HA).

L. Laguarda, S. Hickel, F.F.J. Schrijer, B.W. van Oudheusden (2020)
Journal of Fluid Mechanics 888: A18. doi: 10.1017/jfm.2020.28

The response of asymmetric and planar shock interactions to a continuous excitation of the lower incident shock is investigated numerically. Incident shock waves and centred expansion fans are generated by two wedges asymmetrically deflecting the inviscid free stream flow at Mach 3.

W. Hu, S. Hickel, B.W. van Oudheusden (2019)
Phys. Rev. Fluids 4, 103904. doi: 10.1103/PhysRevFluids.4.103904

The transition mechanism and unsteady behavior behind a backward-facing step (BFS) in the supersonic regime at Ma = 1.7 and Re_δ = 13718 is investigated using large-eddy simulation (LES). The visualization of the flow field shows that the transition process behind the step is initiated by a Kelvin-Helmholtz (K-H) instability of the separated shear layer, followed by secondary modal instabilities of the K-H vortices, leading to lambda-shaped vortices, hair-pin vortices and finally to a fully turbulent state.

V. Pasquariello, S. Hickel, N.A. Adams (2017)
Journal of Fluid Mechanics 828: 617-657. doi: 10.1017/jfm.2017.308

We analyse the low-frequency dynamics of a high Reynolds number impinging shock-wave/turbulent boundary-layer interaction (SWBLI) with strong mean-flow separation. The flow configuration for our grid-converged large-eddy simulations (LES) reproduces recent experiments for the interaction of a Mach 3 turbulent boundary layer with an impinging shock that nominally deflects the incoming flow by 19.6° . The Reynolds number based on the incoming boundary-layer thickness of Re_δ ≈ 203 000 is considerably higher than in previous LES studies.

J. Matheis, S. Hickel (2015)
Journal of Fluid Mechanics 776: 200-234. doi: 10.1017/jfm.2015.319

The reflection of strong oblique shock waves at turbulent boundary layers is studied numerically and analytically. A particular emphasis is put on the transition between regular shock-wave/boundary-layer interaction (SWBLI) and Mach reflection (irregular SWBLI). The classical two- and three-shock theory and a generalised form of the free interaction theory are used for the analysis of well-resolved large-eddy simulations (LES) and for the derivation of stability criteria.

S. Hickel, C.P. Egerer, J. Larsson (2014)
Physics of Fluids 26: 106101. doi: 10.1063/1.4898641

We derive and analyze a model for implicit Large Eddy Simulation (LES) of compressible flows that is applicable to a broad range of Mach numbers and particularly efficient for LESof shock-turbulence interaction. Following a holistic modeling philosophy, physically sound turbulence modeling and numerical modeling of unresolved subgrid scales (SGS) are fully merged, in a manner quite different from that of traditional implicit LES approaches.

J.F. Quaatz, M. Giglmaier, S. Hickel, N.A. Adams (2014)
International Journal of Heat and Fluid Flow 49: 108-115. doi: 10.1016/j.ijheatfluidflow.2014.05.006

Well-resolved Large-Eddy Simulations (LES) of a pseudo-shock system in the divergent part of a Laval nozzle with rectangular cross section are conducted and compared with experimental results. The LES matches the parameter set of a reference experiment. Details of the experiment, such as planar side walls, are taken into account, all wall boundary layers are well-resolved and no wall model is used.

V. Pasquariello, M. Grilli, S. Hickel, N.A. Adams (2014)
International Journal of Heat and Fluid Flow 49: 116-127. doi: 10.1016/j.ijheatfluidflow.2014.04.005

We investigate a passive flow-control technique for the interaction of an oblique shock generated by an 8.8° wedge with a turbulent boundary-layer at a free-stream Mach number of Ma_∞= 2.3 ${Ma}_{\infty} = 2.3$ and a Reynolds number based on the incoming boundary-layer thickness of Re_δ = 60 500 ${Re}_{δ_{0}} = 60.5 \times 10^{3}$ by means of large-eddy simulation (LES).

M. Grilli, S. Hickel, N.A. Adams (2013)
International Journal of Heat and Fluid Flow 42: 79-93. doi: 10.1016/j.ijheatfluidflow.2012.12.006

Results of a large-eddy simulation (LES) of a supersonic turbulent boundary layer flow along a compression–expansion ramp configuration are presented. The numerical simulation is directly compared with an available experiment at the same flow conditions. The compression–expansion ramp has a deflection angle of β = 25°, the free-stream Mach number is Ma_∞ = 2.88, and the Reynolds number based on the incoming boundary layer thickness is Re_δ = 132 840 ${Re}_{δ_{0}} = 132840$ .

M. Grilli, L.S. Chen, S. Hickel, N.A. Adams, S. Willems, A. Gülhan (2012)
AIAA paper 2012-2701. doi: 10.2514/6.2012-2701

We report on an experimental and computational effort to study the interaction of a compressible turbulent boundary layer with an oblique shock wave. A wide range of shock intensities has been considered in the experiments through a variation of the free-stream Mach number.

S. Hickel, E. Touber, J. Bodart, J. Larsson (2012)
Proceedings of the 2012 Summer Program, Center for Turbulence Research, Stanford University.

Wall-models are essential for enabling large-eddy simulations of realistic problems at high Reynolds numbers. The present study is focused on approaches that directly model the wall shear stress, specifically on filling the gap between models based on wall-normal ordinary differential equations (ODEs) that assume equilibrium and models based on full partial differential equations that do not. We develop ideas for how to incorporate non-equilibrium effects (most importantly, strong pressure-gradient effects) in the wall- model while still solving only wall-normal ODEs.

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