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Compressibility charts for gases with different acentric factors and evaluation of the Redlich-Kwong-Soave equation of state

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dc.contributor.author Kouremenos, DA en
dc.contributor.author Antonopoulos, KA en
dc.date.accessioned 2014-03-01T01:08:17Z
dc.date.available 2014-03-01T01:08:17Z
dc.date.issued 1991 en
dc.identifier.issn 0015-7899 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/10393
dc.subject Critical Point en
dc.subject Equation of State en
dc.subject.classification Engineering, Multidisciplinary en
dc.subject.classification Engineering, Mechanical en
dc.subject.other Equations of State--Gases en
dc.subject.other Nomograms--Compressibility en
dc.subject.other Acentric Factor en
dc.subject.other Compressibility Charts en
dc.subject.other Real Gases en
dc.subject.other Gases en
dc.title Compressibility charts for gases with different acentric factors and evaluation of the Redlich-Kwong-Soave equation of state en
heal.type journalArticle en
heal.identifier.primary 10.1007/BF02561416 en
heal.identifier.secondary http://dx.doi.org/10.1007/BF02561416 en
heal.language English en
heal.publicationDate 1991 en
heal.abstract The Redlich-Kwong-Soave generalized equation of state is transformed into a dimensionless form, which permits plotting of one compressibility chart for each value of the acentric factor omega. Such charts are provided for various values of omega in the range omega = 0-0.6. A systematic evaluation of the Redlich-Kwong-Soave equation is made by comparison with the latest version of the generalized compressibility chart given by Nelson and Obert. It is found that for omega = 0, the Redlich-Kwong-Soave compressibility chart agrees well with the Nelson-Obert chart, apart from a small region near the critical point: For values of the reduced pressure p(r) < 1, the relative ercompressibility factor z is less than about 1%. For reduced pressures and temperatures in the ranges 1 less-than-or-equal-to p(r) less-than-or-equal-to 8 and 1 less-than-or-equal-to T(r) less-than-or-equal-to 3.5, respectively, it is found e less-than-or-equal-to 1% at the higher values of T(r), e less-than-or-equal-to 5% at the intermediate T(r) and e less-than-or-equal-to 10% at the lower T(r). The highest disagreement is observed near the critical point (p(r) = T(r) = 1). Moreover, the exact compressibility chart of the real air is developed, based on its exact equation of state, and compared with the Redlich-Kwong-Soave compressibility chart for omega = 0. en
heal.publisher Springer-Verlag en
heal.journalName Forschung im Ingenieurwesen en
dc.identifier.doi 10.1007/BF02561416 en
dc.identifier.isi ISI:A1991GD44000004 en
dc.identifier.volume 57 en
dc.identifier.issue 5 en
dc.identifier.spage 158 en
dc.identifier.epage 161 en


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