74 4.2.1 Pendant une série, p.79 ,
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´ ethanol et le chloroforme ne sont pas dégazés en raison de leurs pressions de vapeur trèstrèsélevées qui les rend trop volatils pourêtrepourêtre pompés ,
eau régale et rincérincéà l'eau ultra-pure, voir § 3.1.4. La cellule prévidée, est ensuite remplie. 5.2.1 ´ Ethanol Nous avons fait la mesure de P cav dans l'´ ethanol dans lapremì ere cellule en pression, o` u P stat est limitélimitéà 3 MPa (voir § 4.1.2) Ainsi les cycles en pression sont composés de 5 P statrégulì erement espacés entre 0 et 3 MPa La température de vaporisation de l'´ ethanol est T b = 78.4 o C lorsque P=0.1 MPa, par conséquent nous nous sommes limitéslimitésà une température expérimentale de 78 o C. On détermine ? aux pressions et températures qui nous intéressent avec l'´ equation (??/?P ) T = 1 /c et c la vitesse du son, et les valeurs tabulées dans les Hand- Books. On a représenté, Fig. 5.1, P stat (?V cav ) pour quelques températures, et P cav (T ) comparé avec les résultats de Ohde et al. Nous obtenons une pression de cavitation légèrement plus négative, maiséloignéemaiséloignée de la théorie. 5.2.2 Chloroforme La série de mesures avec le chloroforme a ´ egalementétéegalementété effectuée dans la pre-mì ere cellule en pression, p.440, 2000. ,
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