Dynamics of spatio-temporal cellular structures by Mutabazi I., et al. (eds.)

Dynamics of spatio-temporal cellular structures by Mutabazi I., et al. (eds.)

By Mutabazi I., et al. (eds.)

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In these films, the observation methods are explained and comments are developed on the analogies between convective motion and the biological phenomena, calling attention on the extraordinary beauty of descriptive physics. It is important to observe that the movies were produced by the Gaumont series on education. In fact, offering movies on craftwork, hygiene, zoology, and physics, L´eon Gaumont considered himself a progressive educator, who thought that cinematography was an important educational support.

The theory was again first developed for stress-free boundary conditions (Malkus and Veronis, 1958 [12]) and later in the no-slip case (Schl¨ uter, Lortz, and Busse, 1965 [38]), both studies concluding for roll patterns. Subsequent developments concerning the stability of the rolls against various secondary mechanisms mainly belong to Busse and Clever [7]. The result is a surface in parameter space called the Busse balloon separating stable roll patterns from unstable ones. In addition to the Rayleigh number, stability depends on the wavelength of the cells and on the Prandtl number.

Des s´eances de la Soci´et´e Fran¸caise de Physique, 1901. 12. H. R. Acad. , 147, 839–842, 9 novembre 1908. 13. H. R. Acad. , 147, 970–972, 23 novembre 1908. 2 Scientific Biography 35 14. H. B´enard, Sur les tourbillons cellulaires, Ann. de Ch. , 8`eme s´erie, 24, 563–566, d´ecembre 1911. 15. H. B´enard, Sur la formation des cirques lunaires, d’apr`es les exp´eriences de C. R. Acad. , 154, 260–263, 29 janvier 1912. 16. H. R. Acad. Sci, 156, 882–884, 17 mars 1913. 17. H. R. Acad. , 156, 1003–1005, 31 mars 1913.

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