首页> 外文期刊>Numerical Heat Transfer, Part B. Fundamentals: An International Journal of Computation and Methodology >DIRECT NUMERICAL SIMULATION OF AIR HEATED CYLINDER WAKE IN TRANSITIONAL STATE, PART III: TEMPERATURE T* IN TURBULENCE ANISOTROPY (TA), TURBULENCE OF T*, DISCONTINUITY AND DISLOCATION B, AND THEIR CAUSES IN T* WITH LAMINAR PSD GRADIENT, PSD OSCILLATION, AND STRONGLY ACTIVE SCALAR
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DIRECT NUMERICAL SIMULATION OF AIR HEATED CYLINDER WAKE IN TRANSITIONAL STATE, PART III: TEMPERATURE T* IN TURBULENCE ANISOTROPY (TA), TURBULENCE OF T*, DISCONTINUITY AND DISLOCATION B, AND THEIR CAUSES IN T* WITH LAMINAR PSD GRADIENT, PSD OSCILLATION, AND STRONGLY ACTIVE SCALAR

机译:过渡状态下空气加热圆柱流的直接数值模拟,第三部分:湍流各向异性(TA)中的温度T *,湍流T *的湍流,不连续性和位移B,以及层状PSD梯度和PSD导致T *的原因强烈活动标量

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摘要

The discontinuity (DC) and dislocation (DL) in a physical property, e.g., temperature T*, besides vortex spiral (SP) [1, 2], are extremely important for wake elucidation, but have not been studied yet. The power spectrum density (PSD) of T* always has a laminar (LA) gradient. Therefore a generation mechanism of DC and DL of T* is extremely different from that in SP [1, 2], and is first elucidated in the present study. Thus a need for presenting the present study is extremely strong. The air-heated wake (HW) at Reynolds number Re=300 and Richardson number Ri=0.3 is generated by three-dimensional (3-D), time-dependent direct numerical simulation (DNS), and arises above a heated horizontal circular cylinder in upward mainstream.The PSD of T* in the HW is composed of the LA-PSD gradient and PSD oscillation. The former cannot generate extreme instability in T*, which arises only in the latter, but is weak.T* has the motion of spanwise velocity w with turbulence. The PSD of T* therefore has PSD oscillation, slight turbulence, and an LA-like state that is PSD with LA gradient and PSD oscillation [with turbulence triggered by strong turbulence anisotropy (strong TA, STA) with w] arising only in the scalar field.Generation of DL in the LA-like state is as follows. A role of STA and w is the turbulence generation in PSD oscillation in T* triggered by STA and w. DL in T* does not arise in LA fluctuation but arises due to turbulence in T* in PSD oscillation.DL is of two kinds. One is DL-A, arising in the transitional region [1, 2] in the SP [2], and having vortex dislocation (VD) [2] in the vector field. The other is DL-B, arising in the LA-like T* due to PSD oscillation in T* in the scalar field.Ri=0.3 is an extremely slight heating rate. The isothermal wake (IW) and HW have similar PSDs of u and v. The T* at Ri=0.3 is a strongly active scalar, and leads to the extremely different PSD of only w from the IW and the suppression of 3-D in the wake.
机译:除了涡旋螺旋(SP)[1、2]以外,物理性质(例如温度T *)中的不连续性(DC)和位错(DL)对于尾波澄清极为重要,但尚未进行研究。 T *的功率谱密度(PSD)始终具有层流(LA)梯度。因此,T *的DC和DL的生成机制与SP中的生成机制极为不同[1,2],并且在本研究中首先进行了阐明。因此,提出本研究的需求非常强烈。雷诺数Re = 300和理查森数Ri = 0.3的风热尾流(HW)是通过三维(3-D)时变直接数值模拟(DNS)生成的,并且出现在加热的水平圆柱体上方硬件中T *的PSD由LA-PSD梯度和PSD振荡组成。前者不能在T *中产生极端不稳定性,后者仅在后者中出现,但很弱。因此T *的PSD具有PSD振荡,轻微的湍流和类似LA的状态,即具有LA梯度和PSD振荡的PSD [由强湍流各向异性(强TA,STA)和w触发的湍流)仅在标量中出现类似于LA的状态下DL的生成如下。 STA和w的作用是由STA和w触发的T *中PSD振荡中的湍流生成。 T *中的DL不是由LA波动引起的,而是由PSD振荡中T *的湍流引起的.DL有两种。一种是DL-A,它出现在SP [2]的过渡区域[1、2]中,并且在矢量场中具有涡旋位错(VD)[2]。另一个是DL-B,由于在标量场中T *中的PSD振荡而在类似LA的T *​​中产生.Ri = 0.3是极小的加热速率。等温尾波(IW)和HW具有相似的u和v PSD.Ri = 0.3处的T *是强活性标量,导致仅w与IW截然不同的PSD和3D的抑制唤醒。

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