Turbulent boundary layers up to Reθ=2500 studied through simulation and experiment
By Philipp Schlatter, Ramis Örlü, Qiang Li, Geert Brethouwer, J. Fransson, Arne V. Johansson, P. Henrik Alfredsson, Dan S. Henningson. 2009
306 citations recorded by the source corpus.
Subfields: Computational Mechanics, Environmental Engineering, Global and Planetary Change
View Paper: https://www.semanticscholar.org/paper/9a09a49711e2adf06b40cfe51fd93931042b5286
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Computational Mechanics
- Ivan Marusic
- B. McKeon
- Javier Jiménez
- Nicholas Hutchins
- Sergio Pirozzoli
- Matteo Bernardini
- Philipp Schlatter
- Alexander J Smits
In Environmental Engineering
- Ivan Marusic
- B. McKeon
- Javier Jiménez
- Nicholas Hutchins
- Sergio Pirozzoli
- Matteo Bernardini
- Philipp Schlatter
- Alexander J Smits
In Global and Planetary Change
- Ivan Marusic
- B. McKeon
- Javier Jiménez
- Nicholas Hutchins
- Alexander J Smits
- Jason Monty
- Sergio Pirozzoli
- Matteo Bernardini
Citations in the corpus
- High–Reynolds Number Wall Turbulence (2011, background): “…& Jiménez 2006, Hutchins & Marusic 2007a,b), and Mathis et al. (2009a) found modulation of the near-wall cycle by long-wavelength motions further from the wall, which is supported by the correlations measured by Tutkun et al. (2009) and the recent simulation results by Schlatter et al. (2009).”
- Turbulence in supersonic boundary layers at moderate Reynolds number (2011, background): “Although still far from values of technological relevance, and accessible in experiments, the Reynolds numbers here attained are sufficient to start observing large-scale influences on the near-wall region (Schlatter et al. 2009).”
- Assessment of direct numerical simulation data of turbulent boundary layers (2010, methodology): “This new DNS is based on the same fully spectral numerical method as used by Schlatter et al. (2009b), and uses the same computational domain as Schlatter et al. (2010).”
- Very-large-scale motions in a turbulent boundary layer (2010, result): “…the fringe method, as did Schlatter et al. (2009), but their computational box 450δ∗|x =0 was much shorter and might not have been sufficient for the full resolution of the turbulent motions, in contrast to those used in the present study (1500δ∗|x =0) and by Schlatter et al. (2009) (3000δ∗|x = 0).”
- Cascades in Wall-Bounded Turbulence (2012, background): “…of the most intriguing discoveries of the 1990s was that even stable perturbations can grow substantially by extracting energy from the mean flow (Schmid 2007) and that it is possible to relate such transient growth to some of the structures of wall-bounded turbulence (Butler & Farrell 1993, del…”
- Three-dimensional conditional structure of a high-Reynolds-number turbulent boundary layer (2011, background): “More recently, Schlatter et al. (2009) have shown a similar pattern for the wall shear stress correlation.”
- Turbulent boundary layers at moderate Reynolds numbers: inflow length and tripping effects (2012, methodology): “For the main part of the present investigation the DNS of a ZPG TBL by Schlatter et al. (2009), here serving as the baseline simulation, was re-simulated, however with different tripping parameters to examine these effects on the turbulent boundary layer developing downstream.”
- Turbulent boundary layers and channels at moderate Reynolds numbers (2010, methodology): “The more recent one by Schlatter et al. (2009), which is comparable to the present one, although at a slightly lower resolution, extends to Reθ = 2500, but the friction Reynolds numbers of even these newer boundary layers (δ+ ≈ 700–800) are still lower than the intermediate channel simulations…”
- History effects and near equilibrium in adverse-pressure-gradient turbulent boundary layers (2017, methodology): “The DNS of ZPG TBL by Schlatter et al. (2009) is considered to provide a baseline case, with respect to which pressure-gradient effects can be assessed, since the APG cases start from the same initial conditions as the ZPG case.”