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 |