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Generation of microbubbles from hollow cylindrical ultrasonic horn
Institution:1. Department of Mechanical Engineering, Transilvania University Brasov, Eroilor 29, 500036 Brasov, Romania;2. IEFA/Physics Department, Transilvania University Brasov, Eroilor 29, 500036 Brasov, Romania;1. Department of Mechanical Engineering, Graduate School of Engineering, Kobe University, 1-1 Rokkodai, Nada, Kobe 657-8501, Japan;2. Housing Systems Business Group, Panasonic Corporation, 1048 Kadoma, Osaka 571-8686, Japan;1. Department of Chemical & Biological Engineering, University of Sheffield, Sheffield, United Kingdom;2. Department of Mechanical Engineering, University of Sheffield, Sheffield, United Kingdom;3. Institute of Thermomechanics AS CR, v.v.i., Czech Academy of Sciences, Prague, Prague, Czech Republic
Abstract:In this study, we found that microbubbles with diameters of less than 100 μm can be easily generated by using a hollow cylindrical ultrasonic horn. Consecutive images of bubbles obtained by using high-speed and high-resolution cameras reveal that a capillary wave is formed on the gas–liquid interface under weak ultrasonic irradiation and that the wave head is detached in the form of bubbles by the fragmentation of the interface as the power of ultrasonic irradiation increases. Moreover, consecutive images of the bubble interface obtained by an ultra-high-speed camera indicate that the breakup of bubbles oscillating harmonically with the ultrasonic irradiation generates many microbubbles that are less than 100 μm in diameter. With regard to the orifice diameter of the horn end, we found that its optimum value varies with the ultrasonic power input. When the orifice diameter is small, the capillary wave generated from the horn end easily propagates all over the gas–liquid interface, thereby starting the generation of microbubbles at a lower ultrasonic power input. When the orifice diameter is large, the capillary wave is attenuated because of viscosity and surface tension. Hence, in this case, microbubble generation from the horn requires a higher ultrasonic power input. Furthermore, the maximum yield of microbubbles via primary and secondary bubble generation can be increased by increasing the gas flow rate.
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