By S. Fauve, S. Aumaitre, P. Abry, J.-F. Pinton, R. Labbe (auth.), Uriel Frisch (eds.)
Advances in Turbulence VII comprises an summary of the kingdom of turbulence study with a few bias in the direction of paintings performed in Europe. It represents a nearly whole number of the invited and contributed papers added on the 7th eu Turbulence convention, subsidized via EUROMECH and ERCOFTAC and arranged via the Observatoire de l. a. Côte d'Azur. New high-Reynolds quantity experiments mixed with new concepts of imaging, non-intrusive probing, processing and simulation supply top quality facts which placed major constraints on attainable theories. For the 1st time, it's been proven, for a category of passive scalar difficulties, why dimensional research occasionally supplies the inaccurate solutions and the way anomalous intermittency corrections could be calculated from first ideas. the amount is therefore geared in the direction of experts within the sector of move turbulence who couldn't attend the convention in addition to anyone drawn to this quickly relocating box.
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Additional resources for Advances in Turbulence VII: Proceedings of the Seventh European Turbulence Conference, held in Saint-Jean Cap Ferrat, France, 30 June – 3 July 1998 / Actes de la Septième Conférence Européenne de Turbulence, tenue à Saint-Jean Cap Ferrat, France, 30 Juin
Introduction Vortex rings have been widely used to study the fundamentals of vortex motion because they are "robust, as well as simpler to generate, analyse, and isolate from end-effects than other configurations" . The wide application of vortex rings to the study of vortical flow structures make it important that experimental results for vortex rings are repeatable and that the effects of generation conditions are understood. Previously there has been disagreement between various groups and between experiment and theory about the value of the circulation of rings .
It is seen that at the tip of the sheets a bulge or rim is formed due to suface tension forces and behind it the liquide is blown up into a a bag forming a membrane by the aerodynamic pressure. For comparison, Fig. I b shows a case of similar M but somewhat larger Weber number, We = 118, where surface tension forces at the tip are of lesser importance. The drop size is noticeably smaller. At large Weber numbers the breakup is in the form of fibers (Hopfinger and Lasheras, 1994; Lasheras et. , 1998) and the drop size is much smaller.
3. Analysis The results of dye visualisation show that for the orifice geometry, the primary region of vorticity generation is near the lip of the orifice, where the vorticity forms a cylindrical sheet. The sheet subsequently rolls up to form a primary vortex ring. Images of dye tracer injected at the piston face also reveal secondary vorticity in the form of secondary rings that are VORTEX RING FORMATION AT AN ORIFICE 17 generated at the piston face and induced at the boundary layer on the wall behind the primary ring.
Advances in Turbulence VII: Proceedings of the Seventh European Turbulence Conference, held in Saint-Jean Cap Ferrat, France, 30 June – 3 July 1998 / Actes de la Septième Conférence Européenne de Turbulence, tenue à Saint-Jean Cap Ferrat, France, 30 Juin by S. Fauve, S. Aumaitre, P. Abry, J.-F. Pinton, R. Labbe (auth.), Uriel Frisch (eds.)