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Characterization of HIFU transducers designed for sonochemistry application: Acoustic streaming
Institution:1. Institut UTINAM/SRS, UMR 6213, CNRS, University of Bourgogne Franche-Comté, Besançon, France;2. Institut FEMTO-ST/ENISYS, UMR 6174, CNRS, University of Bourgogne Franche-Comté, ENSMM, UTBM, Belfort, France;1. Manufacturing and Industrial Processes Research Division, Faculty of Engineering, University of Nottingham Malaysia Campus, 43500 Semenyih, Selangor, Malaysia;2. Department of Chemical and Environmental Engineering, Faculty of Engineering, University of Nottingham Malaysia Campus, 43500 Semenyih, Selangor, Malaysia;1. Manufacturing and Industrial Processes Research Division, Faculty of Engineering, University of Nottingham Malaysia Campus, 43500 Semenyih, Selangor, Malaysia;2. Department of Chemistry, University of Bath, Claverton Down, Bath BA2 7AY, United Kingdom;3. Department of Dentistry, Universiti Kebangsaan Malaysia, Jalan Raja Muda Abdul Aziz, 50300 Kuala Lumpur, Malaysia;1. Atotech Deutschland GmbH, Erasmusstraße 20, 10553 Berlin, Germany;2. Drittes Physikalisches Institut, Georg-August-Universität Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany;1. Polytechnique Montréal – Department of Chemical Engineering, C.P. 6079, Centre Ville, H3C 3A7 Montréal, QC, Canada;2. Università degli Studi di Milano – Chemistry Department, via Golgi 19, 20133 Milan, Italy;3. McGill University – Chemistry Department, 801 Rue Sherbrooke Ouest, Montréal QC H3A 0B8, QC, Canada
Abstract:Cavitation distribution in a High Intensity Focused Ultrasound sonoreactors (HIFU) has been extensively described in the recent literature, including quantification by an optical method (Sonochemiluminescence SCL). The present paper provides complementary measurements through the study of acoustic streaming generated by the same kind of HIFU transducers. To this end, results of mass transfer measurements (electrodiffusional method) were compared to optical method ones (Particle Image Velocimetry). This last one was used in various configurations: with or without an electrode in the acoustic field in order to have the same perturbation of the wave propagation. Results show that the maximum velocity is not located at the focal but shifted near the transducer, and that this shift is greater for high powers. The two cavitation modes (stationary and moving bubbles) are greatly affect the hydrodynamic behavior of our sonoreactors: acoustic streaming and the fluid generated by bubble motion. The results obtained by electrochemical measurements show the same low hydrodynamic activity in the transducer vicinity, the same shift of the active focal toward the transducer, and the same absence of activity in the post-focal axial zone. The comparison with theoretical Eckart’s velocities (acoustic streaming in non-cavitating media) confirms a very high activity at the “sonochemical focal”, accounted for by wave distortion, which induced greater absorption coefficients. Moreover, the equivalent liquid velocities are one order of magnitude larger than the ones measured by PIV, confirming the enhancement of mass transfer by bubbles oscillation and collapse close to the surface, rather than from a pure streaming effect.
Keywords:HIFU  Acoustic streaming  Hydrodynamic behavior  Cavitation  Bubbles behavior
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