dc.creatorUrteaga, Raul
dc.creatorGarcia Martinez, Pablo Luis
dc.creatorBonetto, Fabian Jose
dc.date.accessioned2017-09-15T22:07:14Z
dc.date.available2017-09-15T22:07:14Z
dc.date.created2017-09-15T22:07:14Z
dc.date.issued2009-01
dc.identifierUrteaga, Raul; Garcia Martinez, Pablo Luis; Bonetto, Fabian Jose; Dynamics of sonoluminescing bubbles within a liquid hammer device; American Physical Society; Physical Review E: Statistical Physics, Plasmas, Fluids and Related Interdisciplinary Topics; 79; 1; 1-2009; 1-8; 016306
dc.identifier1063-651X
dc.identifierhttp://hdl.handle.net/11336/24446
dc.identifierCONICET Digital
dc.identifierCONICET
dc.description.abstractWe studied the dynamics of a single sonoluminescing bubble (SBSL) in a liquid hammer device. In particular, we investigated the phosphoric acid–xenon system, in which pulses up to four orders of magnitude brighter than SBSL in water systems (about 1012 photons per pulse)have been previously reported [Chakravarty et al., Phys. Rev. E 69, 066317 (2004)]. We used stroboscopic photography and a Mie scattering technique in order to measure the radius evolution of the bubbles. Under adequate conditions we may position a bubble at the bottom of the tube (cavity) and a second bubble trapped at the middle of the tube (upper bubble). During its collapse, the cavity produces the compression of the liquid column. This compression drives impulsively the dynamics of the upper bubble. Our measurements reveal that the observed light emissions produced by the upper bubble are generated at its second collapse. We employed a simple numerical model to investigate the conditions that occur during the upper bubble collapse. We found good agreement between numerical and experimental values for the light intensity (fluence) and light pulse widths. Results from the model show that the light emission is increased mainly due to an increase in noble gas ambient radius and not because the maximum temperature increases. Even for the brightest pulses obtained (2x1013 photons, about 20 W of peak power) the maximum temperatures computed for the upper bubble are always lower than 20000 K.
dc.languageeng
dc.publisherAmerican Physical Society
dc.relationinfo:eu-repo/semantics/altIdentifier/doi/http://dx.doi.org/10.1103/PhysRevE.79.016306
dc.relationinfo:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pre/abstract/10.1103/PhysRevE.79.016306
dc.rightshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectLiquid
dc.subjectHammer
dc.subjectSonoluminescent
dc.subjectBubble
dc.titleDynamics of sonoluminescing bubbles within a liquid hammer device
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:ar-repo/semantics/artículo
dc.typeinfo:eu-repo/semantics/publishedVersion


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