la moyenne et l'écart-type sont calculés d'après (3.2). sur la figure 3.3, les quantités moyennes (?W ? ou ?U ?) sont tracées la première colonne lorsque les écarts-types associés ,
une baisse de ?W ? est constatée de 120 dv à 180 dv le long de la droite A (Fig. 3.3c), elle est maximale dans la région centrale pour x ? [?B/4 La descente du jet des soupapes est importante au début de l'admission et elle diminue jusqu'au PMB. La figure 3.3c indique une réduction de la fluctuation. Le long de la droite B, la vitesse verticale est très importante à 120 dv lorsque elle est presque nulle au PMB (Fig. 3.3d) De plus, l'écoulement est plus fluctuante au voisinage du piston (Fig. 3.3e). A 270 dv, nous observons que les vitesses sont ascendantes le long des droites A et B (Fig. 3.3b et d). Il est intéressant de remarquer que le long ,
) démontre que l'écoulement tourne dans le sens horaire dans le repère xOz (Fig. 3.3f) De plus, le module de la vitesse moyenne ?U ? se réduit pendant l'admission puis s'amplifie, ceci entraîne une variation de l ,
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