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              <p>Nous avons étudié la convection de Rayleigh Bénard dans une cavité cylindrique de section circulaire dont la hauteur est égale au rayon. En augmentant Ra, la transition est vers un état stationnaire pour Re &amp;lt; 95, et vers des oscillations pour Re &amp;gt; 95. Les cycles limites apparaissent par une bifurcation de Hopf et disparaissent par une bifurcation globale, auquel la période est infinie  La résolution numérique est basée sur la méthode des volumes finis.</p>
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