By S. Fauve, S. Aumaitre, P. Abry, J.-F. Pinton, R. Labbe (auth.), Uriel Frisch (eds.)
Advances in Turbulence VII comprises an outline of the country of turbulence examine with a few bias in the direction of paintings performed in Europe. It represents a virtually entire number of the invited and contributed papers added on the 7th ecu Turbulence convention, subsidized through EUROMECH and ERCOFTAC and arranged by way of the Observatoire de l. a. Côte d'Azur. New high-Reynolds quantity experiments mixed with new ideas of imaging, non-intrusive probing, processing and simulation offer top of the range info which positioned major constraints on attainable theories. For the 1st time, it's been proven, for a category of passive scalar difficulties, why dimensional research occasionally offers the inaccurate solutions and the way anomalous intermittency corrections may be calculated from first rules. the amount is therefore geared in the direction of experts within the region of movement turbulence who couldn't attend the convention in addition to anyone drawn to this speedily relocating box.
Read or Download 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 PDF
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Extra 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
Instantaneous velocity field (a) and corresponding vorticity field (b) of a separated flow over a blunt flat plate. Re = Uvh = 1000, plate thickness = h, X' = I, Y' = fi flow is from left-to-right The spatio-temporal PIV measurements have permitted the determination of the in-plane components of the Reynolds stress tensor in and around the bubble region. Figure 3 shows that the u'v' component is found to peak in the shear layer. This is also the region of largest mean shear and hence, the region of largest energy transfer from the mean flow to the oscillating flow.
Hemisphere Publ. Corp, New York Li, J. (1996) Resolution numerique de l'equation de Navier-Stokes avec reconnection d'interfaces: Methode de suivi de volume et application a l'atomization. These de Doctorat, Univeriste Pierre et Marie Curie, Paris. , Lasheras, lC. and Hopfinger, EJ. (1998) Atomization of a liquid jet by a high momentum coaxial swirling gas jet. 3rd Int. Conf. Multiphase Flow, Lyon. J. (1998) Primary instability of a plane liquid-gas shear layer (submitted to J. ). Raynal, L. (1997) Instabilite et Entrainement al'interface d'une couche de melange Liquide-Gaz.
Thus, secondary effects are important and secondary vorticity must be recognised and accounted for. The effects of secondary vorticity from the piston face can be eliminated by having the piston face finishing position far from the inside wall. Piston face vorticity is of particular concern at high Impulse Ratios since the strength of the secondary ring is a function of the piston stroke length. It should also be noted that the effects of vorticity generated at the piston are not restricted to the impulsively started vortex ring flow.