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Redlick-Kwong » pour modéliser le gaz. En condition limite d'entrée, ils supposent connus l'enthalpie, le débit masse et la vitesse, notre cas, ces informations d'entrées sont inconnues. Aussi, pour en faire abstraction, on inclut le réservoir du gaz en question dans la modélisation ,
A.13) présente les différentes parties du modèle. Pour la suite ,
PS 0 (P, s 0 ) et CS PS 0 (P, s 0 ) à l'aide de la table S PT , H PT et CS PT (Fig.A.15) Ces deux tables nous donnent ainsi l'évolution de l'enthalpie et la célérité du son en fonction de la pression au col. Enfin, on génère la table C PS 0 (P, s 0 ) à l'aide de la table H PS et avec la relation suivante : C PS 0 (P, s 0 ,
(la vanne) en fonction de la pression qui y règne Cette table est dite « décroissante » sur la figure (Fig.A.14) car la vitesse au col diminue lorsque la pression augmente (la détente est moins forte). A l'inverse, vitesse du son qui croit lorsque P augmente au niveau du col (à entropie constante). La dernière étape est de déterminer le point d'intersection (P 1L , C 1L ) de ces deux tables C P S et CS P S ,
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