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Kraichnan-Leith-Batchelor similarity theory and two-dimensional inverse cascades

机译:Kraichnan-Leith-Batchelor相似理论和二维逆级联

摘要

We study the scaling properties and Kraichnan-Leith-Batchelor (KLB) theory of forced inverse cascades in generalized two-dimensional (2D) fluids ($lpha$-turbulence models) simulated at resolution $8192^2$. We consider $lpha=1$ (surface quasigeostrophic flow), $lpha=2$ (2D vorticity dynamics) and $lpha=3$. The forcing scale is well-resolved, a direct cascade is present and there is no large-scale dissipation. Coherent vortices spanning a range of sizes, most larger than the forcing scale, are present for both $lpha=1$ and $lpha=2$. The active scalar field for $lpha=3$ contains comparatively few and small vortices. The energy spectral slopes in the inverse cascade are steeper than the KLB prediction $-(7-lpha)/3$ in all three systems. Since we stop the simulations well before the cascades have reached the domain scale, vortex formation and spectral steepening are not due to condensation effects; nor are they caused by large-scale dissipation, which is absent. One- and two-point pdfs, hyperflatness factors and structure functions indicate that the inverse cascades are intermittent and non-Gaussian over much of the inertial range for $lpha=1$ and $lpha=2$, while the $lpha=3$ inverse cascade is much closer to Gaussian and non-intermittent. For $lpha=3$ the steep spectrum is close to that associated with enstrophy equipartition. Continuous wavelet analysis shows approximate KLB scaling $mathcal{E}(k) propto k^{-2}$ ($lpha=1$) and $mathcal{E}(k) propto k^{-5/3}$ ($lpha=2$) in the interstitial regions between the coherent vortices. Our results demonstrate that coherent vortex formation ($lpha=1$ and $lpha=2$) and non-realizability ($lpha=3$) cause 2D inverse cascades to deviate from the KLB predictions, but that the flow between the vortices exhibits KLB scaling and non-intermittent statistics for $lpha=1$ and $lpha=2$. The results will appear in cite{BurgessEA2015}, which has been accepted to the emph{Journal of Fluid Mechanics}.
机译:我们研究了在分辨率为$ 8192 ^ 2 $的广义二维(2D)流体($ alpha $-湍流模型)中的强制逆级联的缩放性质和Kraichnan-Leith-Batchelor(KLB)理论。我们考虑$ alpha = 1 $(表面准营养流),$ alpha = 2 $(二维涡度动力学)和$ alpha = 3 $。强迫尺度得到很好的解决,存在直接级联并且没有大规模的耗散。对于$ alpha = 1 $和$ alpha = 2 $都存在跨越大小范围的相干涡旋,最强于强迫尺度。 $ alpha = 3 $的活动标量字段包含相对较少的涡旋和较小的涡旋。在所有三个系统中,逆级联中的能谱斜率比KLB预测$-(7- alpha)/ 3 $陡。由于我们在级联达到域尺度之前就已经停止了仿真,因此涡流的形成和频谱的陡峭并不是由于凝结效应引起的。它们也不是由大规模耗散引起的,而这种耗散是不存在的。一点和两点pdf,超平坦度因子和结构函数表明,在$ alpha = 1 $和$ alpha = 2 $的大部分惯性范围内,反向级联是间歇性且非高斯的,而$ alpha = 3 $逆级联更接近于高斯和非间歇性。对于 alpha = 3 $,陡峭的光谱接近与涡旋等分相关的光谱。连续小波分析显示了近似的KLB缩放比例$ mathcal {E}(k) propto k ^ {-2} $($ alpha = 1 $)和$ mathcal {E}(k) propto k ^ {-5 / 3} $($ alpha = 2 $)在相干涡之间的间隙区域中。我们的结果表明,相干涡形成($ alpha = 1 $和$ alpha = 2 $)和不可实现性($ alpha = 3 $)导致2D逆级联偏离KLB的预测,但是之间的流动涡流表现出KLB标度和$ alpha = 1 $和$ alpha = 2 $的非间歇统计量。结果将显示在 cite {BurgessEA2015}中,该目录已被 emph {Journal of Fluid Mechanics}接受。

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