By J. T. Stuart (auth.), Professor Dr. Geneviève Comte-Bellot, Professor Dr. Jean Mathieu (eds.)

Since 1964 the most functionality of the ecu Mechanics Committee has been to rearrange Euromech Colloquia. those are 3- or four-day conferences for the dialogue of present study on a designated and comparatively slim subject in mechanics, through approximately 50 experts selected for his or her energetic involvement in study in that subject. The association of every Euromech Colloquium is entrusted by means of the Committee to 1 or chosen scientists of reputation within the box, and those organizers are enjoined to accomplish a pleasant and casual discussion board for dialogue, with at the very least paper paintings and expenditure. Over 220 Euromech Colloquia were held considering 1964 (about forty each one in France, West Germany and Britain and the remaining in 18 nations in either western and jap Europe) on quite a lot of subject matters drawn from the mechanics of stable fabrics, hydrodynamics, gasoline dynamics and mechanical structures. The Committee believes that jointly, Euromech Colloquia have made an important contribution to the trade of rules on issues in mechanics inside of Europe and feature thereby helped to beat the boundaries to effortless clinical verbal exchange in that sorely divided continent. many years in the past the ecu Mechanics Committee became its atten­ tion to the prospective desire for ecu meetings on a bigger scale than Euromech Colloquia.

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Additional resources for Advances in Turbulence: Proceedings of the First European Turbulence Conference Lyon, France, 1–4 July 1986

Sample text

Configuration of the channels Although the conditions may be specified by the values of R, D and L and by the shape of the channel, we shall show that many flows are possible with the same conditions. We have studied steady and time-periodic flows in the early stages of transition to turbulence, finding, in particular, many bifurcations and multiple equilibria of steady flows. We did numerical experiments for channels of the form illustrated in Fig. 1. Note that the channel is symmetric up and down, by reflection in the centre line, z = 0 say.

0 _ .... - - - - - - - - - - - - - - - - - - - .... 1. ' - - - - . - - - , - - - - - . - - - , - - - - - . 0 Fig. 3. R Calculated bifurcation diagram for the channel with 0 3 and L 80 Note that s = 0 if and only if the flow is symmetric. 3 for o = 3 and L = 80. It can be seen that there are four asymmetric stable steady solutions when R = 20, for example. In fact, the two co-existing asymmetric flows with positive (or negative) s at the same values of R, 0 and L are very simi Jar. SOBEY and DRAZIN [1] have also plotted the stations x where the direction of flow near each wall of the channel changes sign.

Proc. Roy. Soc. A399, 25 (1985) ~, 465 (1985) United Tech. Res. , E. , Rept. A. paper no. 84-1582 (1984) and J. , in press (1986» 4. A. E. Abbott: in Turb. in Internal Flows (ed. B. Murthy), Hemisph. Pub. , Wash. (1977) 5. H. Fasel: Proc. Symp. on Turb. & Chaotic Phen. in Fluids (ed. Tatsumi), Elsevier (1984) 6. A. T. Patera: 7. D. Craik: J. Fluid Mech. 128. 347(1983) Proc. IUTAM Symp. -Turb. transition {ed. V. Kozlov), Springer-Verlag (1985) 8. T. A. Stewart: United Tech. Res. Cent. E. , Rept.

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