TY - GEN
T1 - A DATA-BASED ONE-LAYER FORMULATION OF THE TWO-EQUATION RANS MODELS
AU - Hu, Xiaohan
AU - Huang, George
AU - Kunz, Robert
AU - Yang, Xiang
N1 - Publisher Copyright:
Copyright © 2024 by ASME.
PY - 2024
Y1 - 2024
N2 - The conventional k − ε model accurately predicts the slope of the logarithmic law but falls short in estimating its intercept as well as the buffer layer. This limitation can be addressed either through a two-layer formulation or by introducing additional terms. However, both strategies necessitate extra adjustable constants and ad-hoc functions. In contrast, this paper introduces a novel one-layer k − ε model, which seamlessly integrates the law of the wall while preserving the essential structure of the k − ε framework. Our approach modifies the unclosed dissipation terms in the k and ε equations specifically within the wall layer. We invoke no other assumption than the general law of the wall and the assumptions that led to the k − ε model. Neither do we resort to ad hoc source terms. The revised model yields the following physical scalings in the viscous sublayer: k ∼ y2, ε ∼ y0. In addition, we demonstrate analytically the infeasibility of sustaining the νt ∼ y3 scaling. Beyond the sublayer scalings, our model effectively captures the mean flow characteristics in both the buffer layer and the logarithmic layer, resulting in robust predictions of skin friction for zero-pressure-gradient flat-plate boundary layers and plane channels. To further validate our one-layer formulation, we apply our model to boundary layers under varying pressure gradients and channels experiencing sudden deceleration. Our model’s results closely align with the reference direct numerical simulation and experimental datasets.
AB - The conventional k − ε model accurately predicts the slope of the logarithmic law but falls short in estimating its intercept as well as the buffer layer. This limitation can be addressed either through a two-layer formulation or by introducing additional terms. However, both strategies necessitate extra adjustable constants and ad-hoc functions. In contrast, this paper introduces a novel one-layer k − ε model, which seamlessly integrates the law of the wall while preserving the essential structure of the k − ε framework. Our approach modifies the unclosed dissipation terms in the k and ε equations specifically within the wall layer. We invoke no other assumption than the general law of the wall and the assumptions that led to the k − ε model. Neither do we resort to ad hoc source terms. The revised model yields the following physical scalings in the viscous sublayer: k ∼ y2, ε ∼ y0. In addition, we demonstrate analytically the infeasibility of sustaining the νt ∼ y3 scaling. Beyond the sublayer scalings, our model effectively captures the mean flow characteristics in both the buffer layer and the logarithmic layer, resulting in robust predictions of skin friction for zero-pressure-gradient flat-plate boundary layers and plane channels. To further validate our one-layer formulation, we apply our model to boundary layers under varying pressure gradients and channels experiencing sudden deceleration. Our model’s results closely align with the reference direct numerical simulation and experimental datasets.
UR - http://www.scopus.com/inward/record.url?scp=85204674838&partnerID=8YFLogxK
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U2 - 10.1115/FEDSM2024-130697
DO - 10.1115/FEDSM2024-130697
M3 - Conference contribution
AN - SCOPUS:85204674838
T3 - American Society of Mechanical Engineers, Fluids Engineering Division (Publication) FEDSM
BT - Computational Fluid Dynamics (CFDTC); Micro and Nano Fluid Dynamics (MNFDTC); Flow Visualization
PB - American Society of Mechanical Engineers (ASME)
T2 - ASME 2024 Fluids Engineering Division Summer Meeting, FEDSM 2024 collocated with the ASME 2024 Heat Transfer Summer Conference and the ASME 2024 18th International Conference on Energy Sustainability
Y2 - 15 July 2024 through 17 July 2024
ER -