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Bubble deformation by a turbulent flow

机译:湍流泡沫变形

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We investigate the modes of deformation of an initially spherical bubble immersed in a homogeneous and isotropic turbulent background flow. We perform direct numerical simulations of the two-phase incompressible Navier-Stokes equations, considering a low-density bubble in the high-density turbulent flow at various Weber numbers (the ratio of turbulent and surface tension forces) using the air-water density ratio. We discuss a theoretical framework for the bubble deformation in a turbulent flow using a spherical harmonic decomposition. We propose, for each mode of bubble deformation, a forcing term given by the statistics of velocity and pressure fluctuations, evaluated on a sphere of the same radius. This approach formally relates the bubble deformation and the background turbulent velocity fluctuations, in the limit of small deformations. The growth of the total surface deformation and of each individual mode is computed from the direct numerical simulations using an appropriate Voronoi decomposition of the bubble surface. We show that two successive temporal regimes occur: the first regime corresponds to deformations driven only by inertial forces, with the interface deformation growing linearly in time, in agreement with the model predictions, whereas the second regime results from a balance between inertial forces and surface tension. The transition time between the two regimes is given by the period of the first Rayleigh mode of bubble oscillation. We discuss how our approach can be used to relate the bubble lifetime to the turbulence statistics and eventually show that at high Weber numbers, bubble lifetime can be deduced from the statistics of turbulent fluctuations at the bubble scale.
机译:我们研究了均匀各向同性湍流背景流中初始球形气泡的变形模式。我们对两相不可压缩Navier-Stokes方程进行了直接数值模拟,考虑了不同韦伯数(湍流和表面张力之比)下高密度湍流中的低密度气泡,使用空气-水密度比。我们用球谐分解讨论了湍流中气泡变形的理论框架。我们建议,对于气泡变形的每一种模式,由速度和压力波动的统计数据给出一个强迫项,在相同半径的球体上进行评估。该方法在小变形极限下,将气泡变形与背景湍流速度波动正式联系起来。通过对气泡表面进行适当的Voronoi分解,通过直接数值模拟计算出总表面变形和每个单独模式的增长。我们证明了两个连续的时间区域:第一个区域对应于仅由惯性力驱动的变形,界面变形在时间上呈线性增长,与模型预测一致,而第二个区域来自惯性力和表面张力之间的平衡。两个区域之间的过渡时间由气泡振动的第一瑞利模周期给出。我们讨论了如何使用我们的方法将气泡寿命与湍流统计数据联系起来,并最终表明,在高韦伯数下,气泡寿命可以从气泡尺度的湍流波动统计数据中推导出来。

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