The use of non-cavitating coupling fluids for intensifying sonoelectrochemical processes

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TitreThe use of non-cavitating coupling fluids for intensifying sonoelectrochemical processes
Type de publicationJournal Article
Year of Publication2020
AuteursIslam MHujjatul, Naidji B, Hallez L, Taouil AEt, Hihn J-Y, Burheim OS, Pollet BG
JournalULTRASONICS SONOCHEMISTRY
Volume66
Pagination105087
Date PublishedSEP
Type of ArticleArticle
ISSN1350-4177
Mots-clésAsymmetric cavitation, Coupling fluid, Double cell sonoreactor, Mass transfer, Sonoelectrochemistry
Résumé

For the first time, we have investigated the beneficial effects of non-cavitating coupling fluids and their moderate overpressures in enhancing mass-transfer and acoustic energy transfer in a double cell micro-sonoreactor. Silicon and engine oils of different viscosities were used as non-cavitating coupling fluids. A formulated monoethylene glycol (FMG), which is a regular cooling fluid, was also used as reference. It was found that silicon oil yielded a maximum acoustic energy transfer (3.05 W/cm(2)) from the double jacketed cell to the inner cell volume, at 1 bar of coupling fluid overpressure which was 2.5 times higher than the regular FMG cooling fluid. It was also found that the low viscosity engine oil had a higher acoustic energy value than that of the high viscosity engine oil. In addition, linear sweep voltammograms (LSV) were recorded for the quasi-reversible Fe2+/ Fe3+ redox couple (equimolar, 5 x 10(-3) M) on a Pt electrode in order to determine the mass-transport limited current density (j(lim)) and the dimensionless Sherwood number (Sh). From the LSV data, a statistical analysis was performed in order to determine the contribution of acoustic cavitation in the current density variation vertical bar Delta j vertical bar(average) . It was found that silicon oil at 1 bar exhibited a maximum current density variation, vertical bar Delta j vertical bar(average) of similar to 2 mA/cm(2) whereas in the absence of overpressure, the high viscosity engine oil led to a maximum vertical bar Delta j vertical bar(average) which decreased gradually with increasing coupling fluid overpressure. High viscosity engine oil gave a maximum Sh number even without any overpressure which decreased gradually with increasing overpressure. The Sh number for silicon oil increased with increasing overpressure and reached a maximum at 1 bar of overpressure. For any sonoelectrochemical processes, if the aim is to achieve high mass-transfer and acoustic energy transfer, then silicon oil at 1 bar of overpressure is a suitable candidate to be used as a coupling fluid.

DOI10.1016/j.ultsonch.2020.105087