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L. Fig, A.13) présente les différentes parties du modèle. Pour la suite

. Dans-un-deuxième-temps, 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

C. Cette-table and . Ps, (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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