Large-eddy simulation of low-frequency unsteadiness in a turbulent shock-induced separation bubble
By E. Touber, Neil D. Sandham. 2009
562 citations recorded by the source corpus.
Subfields: Aerospace Engineering, Computational Mechanics
View Paper: https://www.semanticscholar.org/paper/6ec9ab9159a2c6edfe4ef54fe4155111677fe264
How researchers see this paper
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In Aerospace Engineering
- Sergio Pirozzoli
- Neil D. Sandham
- E. Touber
- Stefan Hickel
- Matteo Bernardini
- Venkat Narayanaswamy
- Vito Pasquariello
- Nikolaus A. Adams
In Computational Mechanics
- Sergio Pirozzoli
- Nikolaus A. Adams
- Stefan Hickel
- Johan Larsson
- Neil D. Sandham
- E. Touber
- Sanjiva K. Lele
- Matteo Bernardini
Citations in the corpus
- Differential Reynolds-Stress Modeling for Aeronautics (2015, methodology): “The positive values aroundZ 7–10 mm result from the flappingmotion of the incident shock tip [34] and are therefore not found in the RANS solutions.”
- Transitional shock-wave/boundary-layer interactions in hypersonic flow (2014, unknown): “Details of the governing equations and algorithm can be found in Touber & Sandham (2009) and the references cited therein.”
- Analysis of unsteady behaviour in shockwave turbulent boundary layer interaction (2012, methodology): “…simulations (DNSs) (Adams 2000; Pirozzoli & Grasso 2006; Wu & Martin 2007) and large eddy simulations (LESs) (Loginov, Adams & Zheltovodov 2006; Touber & Sandham 2009) of the † Email address for correspondence: muzio.grilli@aer.mw.tum.de shock/boundary-layer interaction started to appear in…”
- Unsteady effects of strong shock-wave/boundary-layer interaction at high Reynolds number (2017, methodology): “In contrast to previous low Reynolds numerical studies (Adams 2000; Touber & Sandham 2009; Priebe & Martín 2012; Pasquariello et al. 2014), our filtered signal shows the well-known intermittent character typically observed in high Reynolds number experiments, that is, the wall-pressure jumps from…”
- Flow physics and RANS modelling of oblique shock/turbulent boundary layer interaction (2013, methodology): “Touber & Sandham (2009b) and Hadjadj et al. (2010) have previously performed LES computations of the IUSTI experiment near the experimental Reynolds number (Reθ = 5100, based on the momentum thickness, θ ), and Pirozzoli & Bernardini (2011) have recently completed a direct numerical simulation…”
- Direct numerical simulation of transonic shock/boundary layer interaction under conditions of incipient separation (2010, background): “…amplification of Reynolds stresses in the APG region, especially in the mixing layer, where the shedding of vortical structures occurs, as also found by Délery (1983), and for supersonic interactions by Adams (2000), Pirozzoli & Grasso (2006), Wu & Martin (2007) and Touber & Sandham (2009).”
- Confinement effects in shock wave/turbulent boundary layer interactions through wall-modelled large-eddy simulations (2014, methodology): “Furthermore, when spanwise periodicity is used in simulations, Touber & Sandham (2009b) found that the size of the separation bubble varies with the width of the domain: if the computational domain is not sufficiently wide in the spanwise direction, the separation bubble size is over-predicted.”
- Low-order stochastic modelling of low-frequency motions in reflected shock-wave/boundary-layer interactions (2011, methodology): “This does not mean that specific forcing from upstream (see Ganapathisubramani et al. 2007, amongst others) or downstream (see Pirozzoli & Grasso 2006; Robinet 2007; Piponniau et al. 2009; Touber & Sandham 2009b) does not play a role, but that they are not necessary.”
- Low-Frequency Unsteadiness of Shock Wave/Turbulent Boundary Layer Interactions (2014, methodology): “Touber & Sandham (2009) performed large-eddy simulations of the impinging SBLI configuration with an 8◦ shock generator to simulate the experiments by Dupont et al. (2005).”
- A scaling analysis for turbulent shock-wave/boundary-layer interactions (2013, background): “…are still under debate, it has been shown recently that in separated cases, the low-frequency unsteadiness of the separation shock is also fairly independent of the particular geometry of the flow (Dussauge, Dupont & Debiève 2006; Dupont et al. 2006; Wu & Martin 2008; Touber & Sandham 2009b).”