一个波动斑块的非线性扩散和衰变扩散到静止的流体中
Takumi Matsuzawa1,2, Minhui Zhu3,4, Nigel Goldenfeld5
1Department of Physics, James Franck Institute, University of Chicago, Chicago, IL 60637.
概括
这项研究揭示了非强制性流如何衰变并扩散到周围的流体中. 研究人员观察到一个动荡的斑点.
科学领域:
- 流体动力学 流体动力学
- 流研究 流研究
- 非线性动力学是一种非线性动力学.
背景情况:
- 动荡的衰变和扩散是基本的,但不太了解的现象.
- 以前的实验由于边界效应或强的平均流量而面临限制.
- 对于流进化的普遍规律仍然是难以捉摸的.
研究的目的:
- 调查非强制性流衰变和膨胀的内在动态.
- 为了规避传统实验设置的局限性.
- 为了提供一个详细的,空间解决的关于流放松的叙述.
主要方法:
- 使用旋发生器创建局部乱斑块.
- 使用粒子图像速度计观察衰变和膨胀.
- 逻辑时间采样,以捕捉长时间的动态.
主要成果:
- 动荡的斑块最初呈现出扩张和衰变,随后在到达水箱壁时过渡到空间均的衰变.
- 观察到的动态被解释为非线性扩散和非线性衰变的相互作用,与Kolmogorov-Barenblatt方程一致.
- 直接证据支持Kolmogorov-Barenblatt模型是在扩张和衰变阶段发现的.
结论:
- 科尔莫戈罗夫-巴伦布拉特方程准确地描述了观察到的流波动力学.
- 这项研究提供了对非强制性流演变的全面解释.
- 动荡的级联在衰变过程中留下了持久的影响,甚至远离最初的强迫.
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