首页> 外文期刊>International Journal of Multiphase Flow >Numerical study of the oscillations of a non-spherical bubble in an inviscid, incompressible liquid. Part I: free oscillations from non-equilibrium initial conditions
【24h】

Numerical study of the oscillations of a non-spherical bubble in an inviscid, incompressible liquid. Part I: free oscillations from non-equilibrium initial conditions

机译:非球形,不可压缩液体中非球形气泡振荡的数值研究。第一部分:来自非平衡初始条件的自由振荡

获取原文
获取原文并翻译 | 示例
           

摘要

We consider the dynamics of a non-spherical gas bubble undergoing large amplitude oscillations of shape and volume in an inviscid, incompressible fluid. Solutions obtained via either a spectral or boundary-integral technique. The primary objective is to explore the coupling between oscillations of bubble volume and shape, starting from initial conditions where the bubble is either deformed in shape or at a non-equilibrium volume, and the fluid is stationary far from the bubble. For bubbles with a spherical mean shape, we consider conditions that are near 2:1 resonance (as predicted by small amplitude theory). We find that the small deformation theory provides a reasonable estimate of the conditions for shape instability, and of the time scales for resonant interactions between the purely radial and shape modes. However, other features such as the onset of higher order shape modes, or strong departures from Rayleigh-Plesset predictions, are not well approximated by the small amplitude theory. Bubbles which have a non-spherical mean shape exhibit two frequency ranges, corresponding to 2:1 and 1:1 resonance, where Rayleigh-Plesset theory is insufficient to describe the volume response of an oscillating bubble. We also show that purely radial initial conditions can lead to bubble breakup as energy is transferred from purely radial oscillations to shape oscillations.
机译:我们考虑非球形气泡在不粘,不可压缩的流体中经历形状和体积的大幅度振荡的动力学。通过光谱或边界积分技术获得的解。主要目的是探索气泡体积和形状的振荡之间的耦合,从气泡变形或处于非平衡体积的初始条件开始,流体远离气泡处于静止状态。对于球形平均形状的气泡,我们考虑接近2:1共振的条件(由小振幅理论预测)。我们发现,小形变理论为形状不稳定性的条件以及纯粹的径向和形状模式之间的共振相互作用的时间尺度提供了合理的估计。但是,其他特征(例如高阶形状模式的出现或与Rayleigh-Plesset预测的强烈偏离)无法通过小振幅理论很好地近似。具有非球形平均形状的气泡表现出两个频率范围,分别对应于2:1和1:1共振,其中瑞利-普莱塞(Rayleigh-Plesset)理论不足以描述振荡气泡的体积响应。我们还表明,纯粹的径向初始条件会导致气泡破裂,因为能量从纯粹的径向振动转移到形状振动。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号