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Local Dynamics and Statistics of Streamline Segments in Fluid Turbulence

机译:流体湍流中流线段的局部动态和统计

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Based on local extreme points of the absolute value u of the velocity field u_i, streamlines are partitioned into segments as proposed by Wang (J. Fluid. Mech. 648:183-203, 2010). The temporal evolution of the arc length l of streamline segments is analyzed and associated with the motion of the isosurface defined by all points on which the gradient in streamline direction {partial deriv}u/{partial deriv}s vanishes. This motion is diffusion controlled for small segments, while large segments are mainly subject to strain and pressure influences. Due to the non-locality of streamline segments, their temporal evolution is not only a result of slow but also of fast changes, which differ by the magnitude of the jump Δl that occurs within a small time step Δt. The separation of the dynamics into slow and fast changes allows the derivation of a transport equation for the probability density function (pdf) P(l) of the arc length l of streamline segments. While slow changes in the pdf transport equation translate into a convection and a diffusion term when terms up to second order are included, the dynamics of the fast changes yield integral terms. The convection velocity corresponds to the first order jump moment, while the diffusion term includes the second order jump moment. It is theoretically and from DNS data of homogeneous isotropic decaying turbulence at two different Reynolds numbers concluded that the normalized first order jump moment is quasi-universal, while the second order one is proportional to the inverse of the square root of the Taylor based Reynolds number Re_λ~(-1/2). It's inclusion thus represents a small correction in the limit of large Reynolds numbers. Numerical solutions of the pdf equation yield a good agreement with the pdf obtained from the DNS data. It is also concluded on theoretical grounds that the mean length of streamline segments scales with the Taylor microscale rather than with any other turbulent length scale, a finding that can be confirmed from the DNS.
机译:基于速度场U_I的绝对值U的局部极端点,流线被划分为王(J. Fluid. Mech.648:183-203,2010)的段。分析了流线段的弧度L的时间演变,并与由流线方向上的梯度的所有点定义的异位表面的运动相关联,{部分德国} U / {Partiv} U / {Partiv} S消失。这种运动是对小段控制的扩散,而大段主要受应变和压力影响。由于流线段的非局部性,它们的时间进化不仅是慢速而且快速变化的结果,这与在较小的时间步长ΔT发生的跳转ΔL的大小不同。动力学的分离变为慢速和快速变化允许为流线段的弧长L的概率密度函数(PDF)P(L)的传输方程推导出来。虽然PDF传输方程的缓慢变化转换为对流和扩散术语,但是当包括二阶时,快速变化的动态产生积分术语。对流速度对应于第一阶跳跃时刻,而扩散项包括第二阶跳跃时刻。理论上,两种不同的雷诺数的均匀各向同性腐烂湍流的DNS数据得出结论:标准化的第一阶跳动力矩是准通用,而第二阶的第一阶的速度与泰勒基雷诺数的平方根的倒数成比例re_λ〜(-1/2)。因此,它是表示大雷诺数的极限的小校正。 PDF方程的数值解产生与从DNS数据获得的PDF吻合良好的一致性。它还在理论场所结束的是,流线段的平均长度与泰勒微尺度相比,而不是与任何其他湍流长度秤相比,可以从DNS确认的发现。

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