A NEW INTERMITTENCY TRANSPORT EQUATION FOR BYPASS TRANSITION

E. Juntasaro, K. Ngiamsoongnirn, V. Juntasaro
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引用次数: 1

Abstract

The new transport equation for intermittency is developed and proposed in this research work, based on the definition of intermittency and the existing transport equations of laminar and turbulent kinetic energy. Its performance is compared with the two existing transition models used in commercial CFD software: L k model and Reθ γ − model, in case of bypass transition. It is found that the proposed model can accurately predict the mean streamwise velocity in the transition zone. For f C , k and u v ′ ′ − , the proposed model has the same performance as the Reθ γ − model. INTRODUCTION During the last decade, there have been two RANSbased transition models used in commercial CFD software: L k model (Walters and Cokljat, 2008) and Reθ γ − model (Langtry and Menter, 2009). The Reθ γ − model was constructed based on correlations obtained from experimental data so that it is reliable only within a range of flow conditions that the experiment is set up to obtain such correlations. The L k model was developed based on basic physical mechanisms and their interaction to capture the flow transition, e.g. redistribution term (process) to model energy transfer from laminar to turbulent stages so that it is more attractive in such a way that it can be applied to a wider range of flow conditions. However, γ , k and L k are strongly related to each other by the definition of γ . Therefore, their transport equations should be developed in an interconnected manner. This research work is aimed to identify the incomplete modeling scheme of the L k model which requires one more transport equation for γ to complete the relationship among γ , k and L k , according to the definition of γ . Finally, the new transport equation for γ will be developed and proposed here. DERIVATION OF A NEW INTERMITTENCY TRANSPORT EQUATION To begin with, γ or the intermittency of laminar-toturbulent flow transition is defined as the fraction of time in which the flow is turbulent at a fixed point (Schneider, 1995). According to its definition, γ can be formulated as follows:
旁路跃迁的一个新的间歇输运方程
本文在对间歇性的定义和现有的层流动能和湍流动能输运方程的基础上,提出了新的间歇性输运方程。在旁路转捩情况下,将其性能与商用CFD软件中现有的两种转捩模型(L k模型和Reθ γ -模型)进行了比较。结果表明,该模型能较准确地预测过渡区的平均流速。对于f C, k和u v′′−,所提出的模型与Reθ γ−模型具有相同的性能。在过去十年中,商业CFD软件中使用了两种基于ranss的过渡模型:L k模型(Walters和Cokljat, 2008)和Reθ γ -模型(Langtry和Menter, 2009)。Reθ γ−模型是基于从实验数据中获得的相关性构建的,因此只有在为获得这种相关性而设置的实验的流动条件范围内,它才是可靠的。L k模型是基于基本的物理机制和它们之间的相互作用来捕捉流动转变的,例如重新分配项(过程)来模拟从层流到湍流阶段的能量转移,因此它更有吸引力,可以应用于更广泛的流动条件。然而,根据γ的定义,γ, k和k之间是紧密相关的。因此,它们的输运方程应该以相互联系的方式发展。本研究工作的目的是找出L k模型的不完全建模方案,即根据γ的定义,需要一个γ的输运方程来完成γ、k和L k之间的关系。最后,我们将发展并提出新的γ输运方程。首先,γ或层流到湍流过渡的间歇性被定义为流动在固定点处于湍流状态的时间分数(Schneider, 1995)。根据其定义,γ可表示为:
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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