1. First turbulence simulation of flows over wing section at Re=1,000,000
We have conducted well-resolved large-eddy simulations (LESs) of the turbulent flow around a NACA4412 wing section up to a numerically high Reynolds number of 1 million (based on inflow velocity and wing chord length). We carefully designed the numerical setup, including resolution and accuracy requirements, and implemented a relaxation-term-based filter for the LES in Nek5000. The LES results were validated against fully-resolved direct numerical simulations (DNSs) of the same flow case.
2. Data-driven methods for studying turbulence
We have developed a data-driven method for predictions of turbulence quantities in spatially-developing boundary layers. In particular, we employed a system identification approach where high-fidelity numerical data are used to build single and multiple-input linear and non-linear transfer functions. The developed methodology has great potential for implementation in experiments and realistic flow control applications.
3. First high fidelity simulations of pitching airflows at moderately high Reynolds numbers
We have conducted high-fidelity simulations of unsteady wings at two different Reynolds numbers. We studied the unsteady boundary layer transition of a laminar wing undergoing forced pitch oscillations at a moderately high Reynolds number of 750,000. The study lead to the development of a low-dimensional model for the approximation of unsteady aerodynamic loads and a much improved understanding of the origin of non-linear aerodynamic response of unsteady laminar airfoils.
Another study involved the study of unsteady aerodynamics of pitching airfoils at lower Reynolds numbers (Re=100,000) which brought to light the complex dynamical behaviour of unsteady separation bubbles. The study found that unsteady separation bubbles can undergo state changes from convective to absolute instability and that such state changes cause abrupt changes in the boundary-layer characteristics of the airfoil, leading to large variations in aerodynamic loading.
4. Large scale simulations of transition under free-stream turbulence in boundary layers over flat plates and low-pressure turbine blades
We also study effects of the free-stream turbulence characteristic length scales and intensity on the transition in an incompressible flat-plate boundary layer by means of DNS. Computations are performed using the spectral element code Nek5000. Numerically-generated homogeneous isotropic turbulence upstream of the leading edge is designed to imitate the characteristics of the grid-generated turbulence in the wind tunnel experiments. Various combination of levels of the free-stream turbulence intensity and integral length scales are simulated. Turbulence statistics and integral quantities are carefully evaluated showing close agreement with the corresponding experimental data.
Further, we study both the effect of the level of free-stream turbulence and the effect of the upstream wakes on the transition in the flow over low-pressure turbine blades. In a second stage of the study, cylinders moving in front of the leading edge of the turbine are included to model the effect of the wake coming from upstream blade. The flow structures and the receptivity of the flow to continuous forcing by the free-stream turbulence and perturbations at the leading edge have been analysed using Spectral Proper Orthogonal Decomposition (SPOD).
5. Large scale simulations of roughness induced transition on swept wings.
We have investigated, through direct numerical simulations, the combined effects of an isolated roughness element together with the presence of free-stream turbulence on a swept-wing boundary layer. In absence of free-stream turbulence it is possible to observe the presence of stationary crossflow vortices behind the roughness element. For a very low free-stream turbulence level (0.03%), it is possible to observe growing disturbances behind small roughness elements that form turbulent spots while traveling downstream. If the level of free-stream turbulence is increased one order of magnitude, a clear laminar-turbulent transition takes place behind the roughness. This study has helped to understand the high sensitivity of the wake of a roughness element to the level of free-stream turbulence and explaining the experimental observations.