Mechanisms of single bubble cleaning

被引:120
作者
Reuter, Fabian [1 ]
Mettin, Robert [1 ]
机构
[1] Univ Gottingen, Christian Doppler Lab Cavitat & Microeros, Drittes Phys Inst, D-37077 Gottingen, Germany
关键词
Particle removal; Jetting bubbles; Shear flow; Bubble collapse; Cavitation cleaning; Cavitation erosion; INDUCED CELL-LYSIS; CAVITATION-BUBBLE; ACOUSTIC CAVITATION; PRESSURE GENERATION; PARTICLE REMOVAL; KELVIN IMPULSE; LASER; COLLAPSE; BOUNDARY; DYNAMICS;
D O I
10.1016/j.ultsonch.2015.06.017
中图分类号
O42 [声学];
学科分类号
070206 ; 082403 ;
摘要
The dynamics of collapsing bubbles close to a flat solid is investigated with respect to its potential for removal of surface attached particles. Individual bubbles are created by nanosecond Nd:YAG laser pulses focused into water close to glass plates contaminated with melamine resin micro-particles. The bubble dynamics is analysed by means of synchronous high-speed recordings. Due to the close solid boundary, the bubble collapses with the well-known liquid jet phenomenon. Subsequent microscopic inspection of the substrates reveals circular areas clean of particles after a single bubble generation and collapse event. The detailed bubble dynamics, as well as the cleaned area size, is characterised by the non-dimensional bubble stand-off gamma = d/R-max, with d: laser focus distance to the solid boundary, and R-max: maximum bubble radius before collapse. We observe a maximum of clean area at gamma approximate to 0.7, a roughly linear decay of the cleaned circle radius for increasing gamma, and no cleaning for gamma > 3.5. As the main mechanism for particle removal, rapid flows at the boundary are identified. Three different cleaning regimes are discussed in relation to gamma: (I) For large stand-off, 1.8 < gamma < 3.5, bubble collapse induced vortex flows touch down onto the substrate and remove particles without significant contact of the gas phase. (II) For small distances, gamma < 1.1, the bubble is in direct contact with the solid. Fast liquid flows at the substrate are driven by the jet impact with its subsequent radial spreading, and by the liquid following the motion of the collapsing and rebounding bubble wall. Both flows remove particles. Their relative timing, which depends sensitively on the exact gamma, appears to determine the extension of the area with forces large enough to cause particle detachment. (III) At intermediate stand-off, 1.1 < gamma < 1.8, only the second bubble collapse touches the substrate, but acts with cleaning mechanisms similar to an effective small gamma collapse: particles are removed by the jet flow and the flow induced by the bubble wall oscillation. Furthermore, the observations reveal that the extent of direct bubble gas phase contact to the solid is partially smaller than the cleaned area, and it is concluded that three-phase contact line motion is not a major cause of particle removal. Finally, we find a relation of cleaning area vs. stand-off gamma that deviates from literature data on surface erosion. This indicates that different effects are responsible for particle removal and for substrate damage. It is suggested that a trade-off of cleaning potential and damage risk for sensible surfaces might be achieved by optimising gamma. (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:550 / 562
页数:13
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