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arXiv 2401.07501physics.flu-dynphysics.app-ph
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马兰戈尼力与曳力对富汽泡向富气泡转变的影响

Effects of Marangoni and drag forces on the transition from vapor-rich to air-rich bubbles

Kyoko Namura, Takuya Iwasaki, Kaoru Nakajima, Motofumi Suzuki

AI总结:

本文研究非脱气水中局部光热加热下富汽泡向富气泡的转变,揭示曳力与马兰戈尼力随气泡半径的不同标度关系决定气泡运动方向,为稳定形成富汽泡提供条件依据。

摘要:

在本研究中,我们通过局部光热加热非脱气水,研究了富气微泡的形成。当非脱气水被局部加热时,首先形成富汽泡。这些气泡的最大半径约为9 μm,并在振荡和呼出富气泡的同时保持稳定。然而,当呼出的气泡融合并长大时,它们会在热源上重新转变为富汽泡。随后,富汽泡暴露于大量空气中,促使其转变为富气泡。本文通过作用于气泡的流动曳力和温度梯度引起的马兰戈尼力解释了呼出的富气泡的运动。由于曳力与气泡半径成正比,而马兰戈尼力与气泡半径的平方成正比,气泡越大,马兰戈尼力的作用越强。因此,随着气泡长大,它们会逆着富汽泡产生的流动被拉向热源。这些结果有助于更好地理解气泡生长,并确定在非脱气水中稳定形成富汽泡的条件。

英文摘要:

In this study, we investigated the formation of air-rich microbubbles through local photothermal heating of non-degassed water. When non-degassed water is locally heated, vapor-rich bubbles are initially formed. These bubbles have a maximum radius of approximately 9 μm and stabilize while oscillating and exhaling air-rich bubbles. However, when the exhaled bubbles fuse and grow, they revert to vapor-rich bubbles on the heat source. The vapor-rich bubbles are then exposed to a large amount of air, causing them to transition to air-rich bubbles. In this paper, the motion of the exhaled air-rich bubble is explained by the drag force owing to the flow and the Marangoni force owing to the temperature gradient acting on the bubble. Because the drag force is proportional to the bubble radius, and the Marangoni force is proportional to the square of the bubble radius, the larger the bubble, the stronger the effect of the Marangoni force. Thus, as the bubbles grow, they are drawn toward the heat source against the flow created by the vapor-rich bubbles. These results are useful for a better understanding of bubble growth and determining the conditions for the stable formation of vapor-rich bubbles in non-degassed water.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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