Please use this identifier to cite or link to this item: https://scholarbank.nus.edu.sg/handle/10635/66738
DC FieldValue
dc.titlePerturbed Lennard-Jones chain equation of state for polymer liquids
dc.contributor.authorChiew, Y.C.
dc.contributor.authorTing, S.K.H.
dc.contributor.authorLeong, K.K.
dc.date.accessioned2014-06-17T08:33:52Z
dc.date.available2014-06-17T08:33:52Z
dc.date.issued2000-02-01
dc.identifier.citationChiew, Y.C., Ting, S.K.H., Leong, K.K. (2000-02-01). Perturbed Lennard-Jones chain equation of state for polymer liquids. Fluid Phase Equilibria 168 (1) : 19-29. ScholarBank@NUS Repository.
dc.identifier.issn03783812
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/66738
dc.description.abstractThe perturbed Lennard-Jones chain (PLJC) equation of state is formulated based on the first-order variational perturbation theory. The model consists of three parameters, namely, number of segments per chain molecule, m, segment size, σ, and segment energy, ε/k. Given the molecular weight, the PLJC equation was used to quantify the pressure-specific volume-temperature properties of a large number of polymer liquids. Very good agreement was found between the predicted and experimentally measured specific volumes. The accuracy of the PLJC equation of state compares favorably with other polymer equations of state. We further proposed a modification to the PLJC equation to include the molecular weight as a parameter in the equation of state and hence, rendering the modified equation of state, itself molecular weight-independent. This modified perturbed Lennard-Jones chain (mPLJC) model was found to represent experimentally measured data very well.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1016/S0378-3812(99)00329-5
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentCHEMICAL & ENVIRONMENTAL ENGINEERING
dc.description.sourcetitleFluid Phase Equilibria
dc.description.volume168
dc.description.issue1
dc.description.page19-29
dc.description.codenFPEQD
dc.identifier.isiut000085869500002
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