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首页> 外文期刊>PHYSICAL REVIEW E >Transition of the scaling law in inverse energy cascade range caused by a nonlocal excitation of coherent structures observed in two-dimensional turbulent fields
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Transition of the scaling law in inverse energy cascade range caused by a nonlocal excitation of coherent structures observed in two-dimensional turbulent fields

机译:由二维湍流场中观测到的相干结构的非局部激发引起的标定律在逆能量级联范围内的过渡

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We numerically investigate the inverse energy cascade range of two-dimensional Navier-Stokes turbulence.nOur focus is on the universality of the Kolmogorov’s phenomenology. In our direct numerical simulations,ntwo types of forcing processes, the random forcing and the deterministic forcing, are employed besides thensystematically varied numerical parameters.We first calculate the two-dimensional Navier-Stokes equations andnconfirm that results in the quasi steady state are consistent with the classical phenomenology for both types ofnforcing processes. It is also found that the difference in forcing process appears after the inverse energy cascadenrange reaches the system size; the dipole coherent vortices emerge and grow only when the random forcing isnadopted. Then we add a large-scale drag term to the Navier-Stokes equations to obtain the statistically stationarynstate. When the random forcing is used, the scaling exponent of the energy spectrum in the stationary state startsnto differ from the predicted −5/3 in the inverse energy cascade range as the infrared Reynolds number Rednincreases, where Red is defined as kf /kd with the forcing wave number kf and the large-scale drag wave numbernkd . That can be interpreted as a transition phenomenon in which the local maximum vorticity grows like an ordernparameter caused by excitation of strong coherent vortices. Strong coherent vortices emerge and grow after thenquasi steady state and destroy the scaling law when Red is over a critical value. These coherent vortices are notndue to the finite-size effect, unlike the dipole coherent vortices. On the other hand, when the deterministic forcingnis adopted, strong coherent vortices are hardly seen and the −5/3 scaling law holds independently of Red. Wenexamine the cases of the combination of both types of forcing processes and find that formation of such coherentnvortices is sensitive to the mechanism of the external forcing process as well as the numerical parameters. Severalntypes of large-scale drag terms are also tested and their insignificant influence on these qualitative properties isnrevealed.
机译:我们对二维Navier-Stokes湍流的能量级联反比范围进行了数值研究。n我们的重点是研究Kolmogorov现象学的普遍性。在我们的直接数值模拟中,除了系统地改变数值参数外,还采用了两种类型的强迫过程,即随机强迫和确定性强迫。首先计算二维Navier-Stokes方程,然后确认准稳态结果与这两种类型的强制过程的经典现象学。还发现,在逆能量级联范围达到系统大小后,强迫过程出现了差异。仅当采用随机强迫时,偶极相干涡才会出现并增长。然后,我们将一个大型阻力项添加到Navier-Stokes方程中,以获得统计上的稳态。当使用随机强迫时,随着红外雷诺数Redn增加,稳态时能谱的定标指数开始不同于预测的-5/3在逆能量级联范围内,其中Red定义为kf / kd强迫波数kf和大阻力波数nkd。这可以解释为一种过渡现象,在该过渡现象中,局部最大涡度像由强相干涡旋的激发所引起的阶数参数一样增长。当Red超过临界值时,强相干涡旋在准稳态之后出现并生长,并破坏缩放定律。与偶极相干涡不同,这些相干涡不受有限尺寸效应的影响。另一方面,当采用确定性强迫时,几乎看不到强相干涡,并且-5/3缩放定律独立于Red。温尼思研究了两种强迫过程的组合情况,发现这种相干涡的形成对外部强迫过程的机理以及数值参数很敏感。还测试了几种n型大型拖曳项,并揭示了它们对这些定性性质的微不足道的影响。

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    《PHYSICAL REVIEW E 》 |2013年第5期| 1-11| 共11页
  • 作者单位

    Software Cradle Co. Ltd. 3-4-5 Umeda Kita-ku Osaka Japan and Division of Physics and Astronomy Graduate School of ScienceKyoto University Kyoto 606-8502 Japan;

    Division of Physics and Astronomy Graduate School of Science Kyoto University Kyoto 606-8502 Japan;

    Division of Physics and Astronomy Graduate School of Science Kyoto University Kyoto 606-8502 Japan;

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