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Calculation of scalar structure functions from a vortex model of turbulent passive scalar transport

机译:从湍流被动标量传输的涡流模型计算标量结构函数

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A Saffman and Pullin [Phys. Fluids 8, 3072 (1996)] type vortex model for passive scalar structure functions is formulated. The intermittent turbulent fine-scale dynamics in the model is represented by numerical solutions of the advection-diffusion and Navier-Stokes equations in the form of axially strained vortex-scalar structures. The use of these structures is motivated by Pullin and Lundgren's [Phys. Fluids 13, 2553 (2001)] asymptotic strained spiral vortex model of turbulent passive scalar transport. Ensemble-averaged scalar structure functions, of even orders 2-10, are calculated from a range of vortex-scalar structures using Monte Carlo integration. For axisymmetric strained scalar fields, acceptable agreement of the second-order structure function with experimental data reported by Antonia and Van Atta [J. Fluid Mech. 84, 561 (1978)] is obtained. Structure functions are also calculated for a range of passive scalar spiral structures. These are generated by the winding of single and double scalar patches in single strained vortex patches and in merging strained vortices. Power-law scaling of the second- and higher-order structure functions is obtained from cases involving the winding of single scalar patches in an axisymmetric strained vortex patch. The second-order scaling exponents from these cases are in reasonable agreement with Kolmogorov-Oboukhov-Corrsin scaling and the experimental results of Antonia et al. [Phys. Rev. A 30, 2704 (1984)] and Gylfason and Warhaft [Phys. Fluids 16, 4012 (2004)]. However, the higher-order scaling exponents from these cases fall below theoretical predictions and experimental results. Higher-order moments are sensitive to the composition of the vortex-scalar structures, and various improvements are suggested that could enhance the performance of the model. The present approach is promising, and it is the first demonstration that a vortex model using simplified NavierStokes dynamics can produce some scalar structure functions that compare favorably with experimental observations. (c) 2008 American Institute of Physics.
机译:Saffman和Pullin [Phys。建立了被动标量结构函数的Fluids 8,3072(1996)]型涡模型。模型中的间歇湍流精细尺度动力学由对流扩散方程和Navier-Stokes方程的数值解表示,形式为轴向应变涡旋标量结构。这些结构的使用是由Pullin和Lundgren的[Phys。 Fluids 13,2553(2001)]湍流被动标量传输的渐近应变螺旋涡模型。使用蒙特卡洛积分,从一系列涡旋标量结构中计算出偶数为2-10的集合平均标量结构函数。对于轴对称应变标量场,二阶结构函数与Antonia和Van Atta报道的实验数据的可接受一致性[J.流体机械。 84,561(1978)。还为一系列无源标量螺旋结构计算了结构函数。这些是通过将单个和双标量斑片缠绕在单个应变涡斑中以及合并应变涡流中生成的。从涉及将单个标量斑片缠绕在轴对称应变涡形斑片中的情况中,获得了二阶和更高阶结构函数的幂律定标。这些情况下的二阶缩放指数与Kolmogorov-Oboukhov-Corrsin缩放和Antonia等人的实验结果合理地吻合。 [物理Rev. A 30,2704(1984)]和Gylfason and Warhaft [Phys。流体,4012(2004)。但是,这些情况下的高阶缩放指数低于理论预测和实验结果。高阶矩对涡旋标量结构的组成很敏感,并提出了各种改进措施,这些措施可以增强模型的性能。目前的方法是有前途的,并且这是第一个证明,使用简化的NavierStokes动力学的涡流模型可以产生一些标量结构函数,与实验观察结果相比具有优势。 (c)2008年美国物理研究所。

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