Ten Years of Industrial Experience with the SST Turbulence Model

By F. Menter, M. Kuntz, R. Langtry. 2003

3,180 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/107feacb716406055c7aba4bddc3a6e8337c21c1

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Citations in the corpus

Development of DDES and IDDES Formulations for the k-ω Shear Stress Transport Model (2012, methodology): “The governing equations of the SST DDES model read as [2]:”
Numerical Evaluation of Flow and Heat Transfer in Plate-Pin Fin Heat Sinks with Various Pin Cross-Sections (2011, methodology): “Menter [39, 40] proposed the equations for the SST model as”
On the accuracy of turbulence models for CFD simulations of vertical axis wind turbines (2019, background): “The better predictions of theu-basedmodels are attributed to their more accurate near-wall formulation [91,102].”
Towards optimal aerodynamic design of vertical axis wind turbines: Impact of solidity and number of blades (2018, methodology): “This model is developed based on the two-equation SST k-u turbulence model [69,70] which has been further improved to predict the laminar-toturbulent transition for wall-bounded flows.”
Effects of flexibility on the aerodynamic performance of flapping wings (2011, methodology): “The turbulence closure is modeled by Menter’s Shear Stress Transport turbulence model [48,49].”
Towards accurate CFD simulations of vertical axis wind turbines at different tip speed ratios and solidities: Guidelines for azimuthal increment, domain size and convergence (2018, methodology): “Note that the ω-based turbulence models benefit from a y-insensitive formulation which means that the model, based on the y of the cells near the wall, will either opt for the low-Reynolds modeling, to resolve the buffer layer and viscous sublayer near the wall, or for wall functions [61,74,75].”
POD-Galerkin method for finite volume approximation of Navier–Stokes and RANS equations (2016, methodology): “read (for further information about the model parameter and functions, please refer to [49,70,71])  ut + (u · ∇)u = ∇ ·  −pI + (ν + νt )  ∇u + (∇u)T  − 2 3 kI  on [0, T ] x Ω ∇ · u = 0 on [0, T ] x Ω u = (−1, 0) on [0, T ] x Γ1 u = (0, 0) on [0, T ] x Γ2,3,4 u = (0, 0) o”
Review and comparison of methods to model ship hull roughness (2020, methodology): “Turbulence is modelled using SST k-ω [32,33] with quadratic constitutive relations [34] and curvature correction [31,35], a model which has shown good agreement with model scale tests.”
Discovery of Algebraic Reynolds-Stress Models Using Sparse Symbolic Regression (2019, methodology): “in which the production of turbulent kinetic energy is augmented by b ij and bounded following Menter’s limiter [25]”