Experimental Investigation of Lagrangian Coherent Structures and Lobe Dynamics in Perturbed Rayleigh-Benard Convection

Masahito Watanabe, Hiroaki Yoshimura
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Abstract

It is well known that Rayleigh-Benard convection with perturbations yields Lagrangian chaotic transport, and the mechanism of inducing chaotic transport has been numerically clarified by lobe dynamics [2]. On the other hand, the mechanism of such Lagrangian transport has not been enough studied by experiments. In our previous work [16], we made an experimental study to investigate the Lagrangian transport appeared in the two-dimensional Rayleigh-Benard convection by giving oscillation on the velocity fields and showed that there exist Lagrangian Coherent Structures (LCSs) which correspond to invariant manifolds of non-autonomous systems. We also showed that the LCSs entangle with each other around cell boundaries. In this paper, we further explore the global invariant structures of the perturbed Rayleigh-Benard convection by clarifying the details on the LCSs and explain how the fluid transport obeys lobe dynamics. Finally, we propose a novel Hamiltonian model for the two-dimensional perturbed Rayleigh-Benard convection that enables to elucidate the global structures detected by experiments.
微扰瑞利-贝纳德对流中拉格朗日相干结构和叶瓣动力学的实验研究
众所周知,具有扰动的瑞利-贝纳德对流产生拉格朗日混沌输运,其诱导混沌输运的机理已经通过叶状动力学在数值上得到了阐明[2]。另一方面,这种拉格朗日输运的机理还没有得到足够的实验研究。在我们之前的工作[16]中,我们通过实验研究了二维瑞利-贝纳德对流中出现的拉格朗日输运,通过对速度场进行振荡,证明了存在拉格朗日相干结构(LCSs),它对应于非自治系统的不变流形。我们还发现lcs在细胞边界周围相互缠绕。在本文中,我们进一步探讨了微扰瑞利-贝纳德对流的全局不变结构,并解释了流体输运如何服从叶状动力学。最后,我们提出了一个新的二维扰动瑞利-贝纳德对流的哈密顿模型,该模型能够解释实验检测到的全局结构。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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