Turkish Journal of Mathematics and Computer Science

Turkish Journal of Mathematics and Computer Science

Comparative Study of Algebraic Wall Model and Differential Equation Wall Model in Large Eddy Simulation of Turbulent Channel Flow

Yazarlar: Muhammad Saiful İslam MALLİK, Mohammad Azizul HOQUE, Md. Ashraf UDDİN

Cilt 9 , Sayı - , 2018 , Sayfalar 80 - 90

Konular:-

Anahtar Kelimeler:Large eddy simulation,Turbulent channel flow,Algebraic wall model

Özet: A large eddy simulation (LES) is performed in a plane turbulent channel flow, where the near wall region is approximated by algebraic wall model (AWM) and differential equation wall model (DEWM). The simulation is performed by using a finite difference method of second order accuracy in space and a low-storage explicit Runge-Kutta method with third order accuracy in time. The computational results are compared with those from direct numerical simulation (DNS) data. Comparing the results throughout the calculation domain we have found that the results from the LES with DEWM (LES-DEWM) approach show closer agreement with the DNS results.


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BibTex
KOPYALA
@article{2018, title={Comparative Study of Algebraic Wall Model and Differential Equation Wall Model in Large Eddy Simulation of Turbulent Channel Flow}, volume={9}, publisher={Turkish Journal of Mathematics and Computer Science}, author={Muhammad Saiful İslam MALLİK,Mohammad Azizul HOQUE,Md. Ashraf UDDİN}, year={2018}, pages={80–90} }
APA
KOPYALA
Muhammad Saiful İslam MALLİK,Mohammad Azizul HOQUE,Md. Ashraf UDDİN. (2018). Comparative Study of Algebraic Wall Model and Differential Equation Wall Model in Large Eddy Simulation of Turbulent Channel Flow (Vol. 9, pp. 80–90). Vol. 9, pp. 80–90. Turkish Journal of Mathematics and Computer Science.
MLA
KOPYALA
Muhammad Saiful İslam MALLİK,Mohammad Azizul HOQUE,Md. Ashraf UDDİN. Comparative Study of Algebraic Wall Model and Differential Equation Wall Model in Large Eddy Simulation of Turbulent Channel Flow. Turkish Journal of Mathematics and Computer Science, 2018, pp. 80–90.