Characterization of the acoustic cavitation in ionic liquids in a horn-type ultrasound reactor

被引:13
作者
Schieppati, Dalma [1 ]
Mohan, Mood [2 ,3 ,4 ]
Blais, Bruno [1 ]
Fattahi, Kobra [1 ]
Patience, Gregory S. [1 ]
Simmons, Blake A. [2 ,5 ]
Singh, Seema [2 ]
Boffito, Daria C. [1 ]
机构
[1] Ecole Polytech Montreal, Dept Chem Engn, CP 6079,Succ CV, Montreal, PQ H3C 3A7, Canada
[2] Joint BioEnergy Inst, Deconstruct Div, 5885 Hollis St, Emeryville, CA 94608 USA
[3] Oak Ridge Natl Lab, Biosci Div, Oak Ridge, TN 37831 USA
[4] Oak Ridge Natl Lab, Ctr Mol Biophys, Oak Ridge, TN 37831 USA
[5] Lawrence Berkeley Natl Lab, Biol Syst & Engn Div, 1 Cyclotron Rd, Berkeley, CA 94720 USA
基金
加拿大自然科学与工程研究理事会;
关键词
Ultrasound; Acoustic pressure; Ionic liquid; Cavitation; Acoustic streaming; Active region; HEAT-CAPACITIES; SONOLUMINESCENCE; TEMPERATURE; SONOCHEMISTRY; VISCOSITY; ESTERIFICATION; DYNAMICS; DENSITY; FLOW;
D O I
10.1016/j.ultsonch.2023.106721
中图分类号
O42 [声学];
学科分类号
070206 ; 082403 ;
摘要
Most ultrasound-based processes root in empirical approaches. Because nearly all advances have been conducted in aqueous systems, there exists a paucity of information on sonoprocessing in other solvents, particularly ionic liquids (ILs). In this work, we modelled an ultrasonic horn-type sonoreactor and investigated the effects of ultrasound power, sonotrode immersion depth, and solvent's thermodynamic properties on acoustic cavitation in nine imidazolium-based and three pyrrolidinium-based ILs. The model accounts for bubbles, acoustic impedance mismatch at interfaces, and treats the ILs as incompressible, Newtonian, and saturated with argon. Following a statistical analysis of the simulation results, we determined that viscosity and ultrasound input power are the most significant variables affecting the intensity of the acoustic pressure field (P), the volume of cavitation zones (V), and the magnitude of the maximum acoustic streaming surface velocity (u). V and u increase with the increase of ultrasound input power and the decrease in viscosity, whereas the magnitude of negative P decreases as ultrasound power and viscosity increase. Probe immersion depth positively correlates with V, but its impact on P and u is insignificant. 1-alkyl-3-methylimidazolium-based ILs yielded the largest V and the fastest acoustic jets - 0.77 cm3 and 24.4 m s-1 for 1-ethyl-3-methylimidazolium chloride at 60 W. 1-methyl-3-(3-sulfopropyl)-imidazolium-based ILs generated the smallest V and lowest u - 0.17 cm3 and 1.7 m s-1 for 1-methyl-3-(3-sulfopropyl)-imidazolium p-toluene sulfonate at 20 W. Sonochemiluminescence experiments validated the model.
引用
收藏
页数:14
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