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, Changement de direction par diiusion d'un chemin optique, p.65

, GGommtrie 1D du mur plan en milieu gris diiusant d e faaon isotrope, p.67

, Domaine de calcul et maillage utilisss pour calculer la amme, p.77

, Comparaison des champs de temprature en K issus de deux calculs eullriens avec gauche et sans droite prise en compte des transferts radiatifs, p.80

, Champs d''nergie cinntique turbulente moyenne gauche et de son taux moyen de dissipation droite issus du calcul eullrien ; hki max ' 25 m 2 s 2 et h k i max ' 10 5 m 2 s 3

, Evolutions en fonction de la richesse des tempratures de trois particules uides typiques suivies lors du calcul lagrangien

.. .. Courbe-d''quilibre-de-temprature-retenue,

, Courbes d''quilibre de fractions molaires d'H 2 O et de CO 2 retenues, p.85

, Courbe d''quilibre de fraction molaire de CO retenue

, Evolutions en fonction de la richesse des fractions volumiques de suie des trois particules uides dont les volutions de temprature sont reprrsenttes sur

, de temprature moyenne, de fraction volumique moyenne de suie et de fractions molaires moyennes de H 2 O et de CO 2 reconstruits partir de la PDF f t r; f V obtenue lors de la simulation lagrangienne, Prools radiaux, 50 cm de hauteur au-dessus du brrleur

, Champs de temprature moyenne en K, gauche et de fraction volumique moyenne de suie droite reconstruits partir de la PDF f t r; f V obtenue lors de la simulation lagrangienne, p.89

, Champs de fraction molaire moyenne de H 2 O gauche et de CO 2 droite reconstruits partir de la PDF f t r; f V obtenue lors de la simulation lagrangienne ; hx H 2 O i max ' 0,12 et hx C O 2 i max ' 0,10

, DDDnition de l''chelle de longueur inttgrale de la turbulence, p.94

, Champs de puissance radiative volumique moyenne en WWm 3 , gauche et de l''cart type correspondant en WWm 3 , droite, obtenus avec la mmthode FM-NUD calcul rraliss avec 10 7 chemins optiques sans prendre en compte l'interaction rayonnementtturbulence

, Champs de puissance radiative volumique moyenne en WWm 3 , gauche et de l''cart type correspondant en WWm 3 , droite, obtenus avec la mmthode ERM-NUD calcul rraliss avec 10 7 chemins optiques sans prendre en compte l'interaction rayonnementtturbulence

, de la puissance radiative volumique moyenne et de l''cart type correspondant, obtenus avec les deux mmthodes donnant les meilleurs rrsultats calcul rraliss avec 10 7 chemins optiques sans prendre en compte l'interaction rayonnementtturbulence, Prools radiaux, 50 cm de hauteur au-dessus du brrleur, p.104

C. , GGommtrie monodimensionnelle du mur plan

, RRle des miroirs sur les plans lattraux

, 50 2.2 Flux averaged over the two walls and, in parentheses, corresponding standard deviation

, Best approaches for radiative p o wer and wall ux calculations, p.57

, Prrsentation des diiirents cas de validation en ux

, Comparaison des ux obtenus par les mmthodes de Monte Carlo directe FM et rrciproques ERM et ARM avec ceux donnns par la solution de rrffrence de Lii et zisik 1911 dans le cas du mur plan pour diiirentes conditions, p.69

, Comparaison des ux obtenus par les mmthodes de Monte Carlo directe FM et rrciproque ARM avec ceux donnns par une mmthode des ordonnnes discrrtes 1D 11 dans le cas du mur plan pour diiirentes conditions, p.70

, Comparaison des puissances radiatives volumiques en WWm 3 obtenues par la mmthode de Monte Carlo rrciproque ERM avec celles issues de l'approximation conductive dans le cas du mur plan optiquement pais

, Conditions imposses sur les frontiires du domaine pour eeectuer le calcul aarothermochimique de la amme

, Conditions imposses sur les frontiires du domaine pour eeectuer le calcul de transferts radiatifs au sein de la amme

, Comparaison des rrsultats obtenus avec les trois mmthodes associies chacune aux deux techniques de rrpartition les deux calculs ont tt rralisss avec 10 7 chemins optiques sans prendre en compte l'interaction rayonnementtturbulence, p.100

, derriire les frontiires ouvertes rrsultats ne prenant pas en compte l'interaction rayonnementtturbulence obtenus avec la mmthode FM-NUD et 10 7 chemins optiques, p.105

, Innuence de la prise en compte de l'interaction rayonnementtturbulence sur les rrsultats obtenus avec la mmthode FM-NUD et 10 7 chemins optiques, p.106

, Innuence de la constante K s du coeecient d'absorption des suies en fonction de la prise en compte ou non de l'interaction rayonnementtturbulence rrsultats obtenus avec la mmthode FM-NUD et 10 7 chemins optiques, p.108

, Innuence de la taille des tourbillons dans la moddlisation de l'interaction rayonnementtturbulence rrsultats obtenus avec la mmthode FM-NUD et 10 7 chemins optiques

, Contribution des gaz et des suies en fonction de la prise en compte ou non de l'interaction rayonnementtturbulence rrsultats obtenus avec la mmthode FM-NUD et 10 7 chemins optiques