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The Growth and Collapse of a Bubble between Parallel Flat Free Surfaces

机译:平行平面自由表面之间的泡沫的生长和崩溃

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The growth and collapse of a bubble between two parallel flat free surfaces and the corresponding water column formation on the free surfaces have been investigated experimentally and numerically. In the experiment, a laser-induced bubble generated inside a plane water jet and the dynamical motion of free surfaces were observed with a high-speed video camera. The results are characterized by two dimensionless parameters: the ratio of the maximum bubble radius to the water jet width, R_(max), and the ratio of the initial bubble offset from the center line of the jet to the water jet width, ε~*. When a bubble is generated at the center (ε~* = 0), water columns are formed on both free surfaces during the growth phase of a bubble, following the formation of crown-like shaped water columns during the second growth and collapse of a bubble. Since the bubble does not translates, it grows and collapses at the center of the jet. However, a water column due to the bubble growth when ε~*≠ 0 tends to be formed only on the nearer free surface to the bubble during its growth phase. Then in the collapse phase the bubble translates toward the other free surface far from the bubble accompanying with a liquid-jet formation toward it. The liquid-jet and the rebound Shockwave from the bubble cause the water column formation on both sides of free surfaces. Numerical simulations are conducted for the growth and collapse phases using the boundary element method (BEM) and for the collapse phase using the ghost fluid method (GFM). The water column formation during the growth phase, a toroidal bubble deformation during the collapse phase, and the translation of the collapsing bubble are well simulated by BEM. The result of GFM shows Shockwave emission from the rebounding motion of the bubble which causes the water column formation when the Shockwave impacts on the free surface with large curvature.
机译:在实验和数值上研究了两个平行的平坦自由表面和自由表面上的相应水柱形成之间的泡沫的生长和崩溃。在实验中,用高速摄像机观察到在平面水射流内产生的激光诱导的气泡和自由表面的动态运动。结果的特征在于两个无量纲参数:最大气泡半径与水射流宽度的比率,R_(最多)和初始气泡与喷射中心线的比率与水射流宽度,ε〜 *。当在中心(ε〜* = 0)产生气泡时,在第二次生长期间形成冠状形状的水柱后,在气泡的生长阶段,在两个自由表面上形成水柱。气泡。由于气泡不转换,因此它在喷射器的中心生长并坍塌。然而,由于ε〜*≠0倾向于在其生长阶段期间仅在更容易自由表面上形成ε-*≠0时,水柱。然后在崩解阶段,气泡朝向远离液体喷射形成的气泡的另一个自由表面转化为其。来自气泡的液体射流和反弹冲击波导致自由表面两侧的水柱形成。使用幽灵流体方法(GFM)使用边界元法(BEM)和塌陷阶段进行数值模拟。在生长阶段期间的水柱形成,塌陷阶段期间的环形气泡变形,并且通过BEM模拟塌陷泡的翻译。 GFM的结果显示了气泡的反弹运动的冲击波发射,当冲击波对具有大曲率的自由表面的冲击产生时导致水柱形成。

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