{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2024,7,27]],"date-time":"2024-07-27T13:13:57Z","timestamp":1722086037979},"reference-count":19,"publisher":"Acoustical Society of America (ASA)","issue":"3","content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"short-container-title":[],"published-print":{"date-parts":[[2008,9,1]]},"abstract":"<jats:p>An experimental study of the extinction threshold of single bubble sonoluminescence in an air-water system is presented. Different runs from 5% to 100% of air concentrations were performed at room pressure and temperature. The intensity of sonoluminescence (SL) and time of collapse (tc) with respect to the driving were measured while the acoustic pressure was linearly increased from the onset of SL until the bubble extinction. The experimental data were compared with theoretical predictions for shape and position instability thresholds. It was found that the extinction of the bubble is determined by different mechanisms depending on the air concentration. For concentrations greater than \u223c30%\u201340% with respect to the saturation, the parametric instability limits the maximum value of R0 that can be reached. On the other hand, for lower concentrations, the extinction appears as a limitation in the time of collapse. Two different mechanisms emerge in this range, i.e., the Bjerknes force and the Rayleigh\u2013Taylor instability. The bubble acoustic emission produces backreaction on the bubble itself. This effect occurs in both mechanisms and is essential for the correct prediction of the extinction threshold in the case of low air dissolved concentration.<\/jats:p>","DOI":"10.1121\/1.2903854","type":"journal-article","created":{"date-parts":[[2008,9,19]],"date-time":"2008-09-19T15:31:41Z","timestamp":1221838301000},"page":"1490-1496","update-policy":"http:\/\/dx.doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":7,"title":["Experimental study of transient paths to the extinction in sonoluminescence"],"prefix":"10.1121","volume":"124","author":[{"given":"Ra\u00fal","family":"Urteaga","sequence":"first","affiliation":[{"name":"Instituto Balseiro-CAB-CONICET Laboratorio de Cavitaci\u00f3n y Biotecnolog\u00eda, , R8402AGP\u2013Av. Bustillo Km. 9,5\u2013San Carlos de Bariloche-R\u00edo Negro, Argentina"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Dami\u00e1n","family":"Dellavale","sequence":"additional","affiliation":[{"name":"Instituto Balseiro-CAB-CONICET Laboratorio de Cavitaci\u00f3n y Biotecnolog\u00eda, , R8402AGP\u2013Av. Bustillo Km. 9,5\u2013San Carlos de Bariloche-R\u00edo Negro, Argentina"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Gabriela F.","family":"Puente","sequence":"additional","affiliation":[{"name":"Instituto Balseiro-CAB-CONICET Laboratorio de Cavitaci\u00f3n y Biotecnolog\u00eda, , R8402AGP\u2013Av. Bustillo Km. 9,5\u2013San Carlos de Bariloche-R\u00edo Negro, Argentina"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Fabi\u00e1n J.","family":"Bonetto","sequence":"additional","affiliation":[{"name":"Instituto Balseiro-CAB-CONICET Laboratorio de Cavitaci\u00f3n y Biotecnolog\u00eda, , R8402AGP\u2013Av. 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