首页> 外文会议>IUTAM Symposium on Elementary Vortices and Coherent Structures >DYNAMICS OF SMALL-SCALE VORTICITY AND STRAIN-RATE STRUCTURES IN THE TRANSITION FROM ISOTROPIC TO SHEAR TURBULENCE
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DYNAMICS OF SMALL-SCALE VORTICITY AND STRAIN-RATE STRUCTURES IN THE TRANSITION FROM ISOTROPIC TO SHEAR TURBULENCE

机译:从各向同性抗剪切湍流从各向同性转变的小规模涡度和应变率结构的动态

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Local topological and statistical measures of enstrophy and strain-rate structures are compared with global statistics to determine the effects of mean shear on the interactions between fluctuating vorticity and strain rate in DNS of transition-ing isotropic to shear turbulence. "Structures" are extracted as concentrations of turbulence fluctuations, allowing quantitative with visual analysis. We find that mean shear adjusts the alignment of fluctuating vorticity and strain rate so as to (1) enhance global and local alignments between vorticity and the second eigenvector of fluctuating strain rate, (2) two-dimensionalize fluctuating strain rate, and (3) align the compressional components of fluctuating and mean strain rate. Shear causes amalgamation of structures and suppresses strain-rate structures between enstrophy structures. Shear enhances "passive" strain-rate fluctuations-strain rate kinemalically induced by local vorticity concentrations with negligible enstrophy production-relative to "active," or vorticity-generating, strain-rate fluctuations. Enstrophy structures separate into "active" and "passive" based on the second eigenvalue of fluctuating strain rate. The time evolution of a shear-induced hairpin enstrophy structure was analyzed. The structure originated in the initial isotropic state as a vortex sheet, evolved into a vortex tube during a transitional period, and developed into a well-defined horseshoe vortex in the shear-dominated state.
机译:将敌意和应变率结构的局部拓扑和统计措施与全局统计数据进行比较,以确定平均剪切对转型各向同性转变各向同性的DNS在剪切湍流中的波动涡度和应变率之间的相互作用的影响。 “结构”被提取为湍流波动的浓度,允许定量与视觉分析。我们发现平均剪切调节波动涡度和应变速率的对准,以便(1)增强涡流与波动应变率的第二特征向量之间的全局和局部对准,(2)二维波动率应变率,(3)对齐波动和平均应变率的压缩组件。剪切导致结构的胺合并并抑制野营结构之间的应变率结构。剪切增强“被动”应变速率波动 - 应变速率,以局部涡流浓度在一起,具有可忽略不计的敌意生产 - 相对于“活性”或涡流产生的应变率波动。基于波动应变率的第二特征值,敌对结构分离为“活跃”和“被动”。分析了剪切诱导的发夹野兽结构的时间演变。在过渡时段期间,该结构源于初始各向同性状态作为涡流,在过渡时期进化成涡流管,并在剪切主导状态下开发成明确定义的马蹄形涡流。

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