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• NACA0012 numerical schemes variation by Michael Alletto
  ...uation, the convective therms in the other equations (energy, momentum and turbulence) are sequantially switched from a second order upstream (the case were all
  4 KB (644 words) - 08:53, 6 January 2022
• Tutorials
  ...ganized into individual topics (e.g. basics, meshing, multiphase modeling, turbulence modeling, programming etc.)
  6 KB (826 words) - 07:57, 15 December 2023
• NACA0012 grid dependence study by Michael Alletto
  [1] Jack R Edwards and Suresh Chandra. Comparison of eddy viscositytransport turbulence models for three-dimensional, shock-separated flowfields. AIAA journal, 34(
  6 KB (925 words) - 08:53, 6 January 2022
• Settling Sphere Contact Angle by Michael Alletto
  ...ains laminar (see [1] for experiments around a sphere). This means that no turbulence model has to be used. For this reason, the main difference to the previous
  9 KB (1,385 words) - 05:46, 1 February 2024
• Dynamic stall NACA0012 Michael Alletto
  ...ee https://www.openfoam.com/documentation/guides/latest/doc/guide-bcs-wall-turbulence-nutkWallFunction.html. Zhi Tao. Turbulence modeling of deep dynamic stall at relatively low
  16 KB (2,279 words) - 20:51, 31 January 2024
• AMR supersonic sphere Re300 Ma1dot2 by Michael Alletto
  ...here, the wall distance can be used to shield the wall layers. Most of the turbulence models have a member function to assess this field (it is called y()).
  22 KB (2,982 words) - 05:48, 1 February 2024

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