Matches in SemOpenAlex for { <https://semopenalex.org/work/W2952011103> ?p ?o ?g. }
- W2952011103 endingPage "71" @default.
- W2952011103 startingPage "59" @default.
- W2952011103 abstract "The capillary effect caused by the confinement in porous media leads to strongly differences in the physical properties and phase equilibrium of the fluids apart from the bulk phase. A joint model was established for investigating the capillary effect by combining Young-Laplace equation and the square-well chain-like fluid with variable well-width range (SWCF-VR) equation of state. The Young-Laplace equation supplies a simple way to relate the capillarity with the bulk properties, and the SWCF-VR equation was able to accurately describe the equilibrium of fluid in bulk phase compared with the Peng–Robinson equation. The model could predict well the phase equilibrium when comparing with experimental data in bulk, and consequently the results for confined fluids. The model was verified by experimental and computer simulation data. Further, the binary adjustable parameters of SWCF-VR EOS used in this study could be updated once the experimental data in confined situation are reported. In addition, the model could be used for complex component when experimental data are unavailable since the four parameters of EOS could be predicted." @default.
- W2952011103 created "2019-06-27" @default.
- W2952011103 creator A5015464400 @default.
- W2952011103 creator A5039032609 @default.
- W2952011103 creator A5044409195 @default.
- W2952011103 creator A5070057968 @default.
- W2952011103 date "2019-10-01" @default.
- W2952011103 modified "2023-09-26" @default.
- W2952011103 title "A joint model for calculating capillary pressure of confined fluid based on the SWCF-VR equation of state" @default.
- W2952011103 cites W1652711717 @default.
- W2952011103 cites W1991084717 @default.
- W2952011103 cites W1991334430 @default.
- W2952011103 cites W1993895687 @default.
- W2952011103 cites W2000293817 @default.
- W2952011103 cites W2004951835 @default.
- W2952011103 cites W2007837872 @default.
- W2952011103 cites W2008947156 @default.
- W2952011103 cites W2011735488 @default.
- W2952011103 cites W2012989857 @default.
- W2952011103 cites W2013229454 @default.
- W2952011103 cites W2019013919 @default.
- W2952011103 cites W2024570634 @default.
- W2952011103 cites W2030472957 @default.
- W2952011103 cites W2034086491 @default.
- W2952011103 cites W2036281599 @default.
- W2952011103 cites W2047144078 @default.
- W2952011103 cites W2050128141 @default.
- W2952011103 cites W2058046601 @default.
- W2952011103 cites W2058305577 @default.
- W2952011103 cites W2062255538 @default.
- W2952011103 cites W2063511737 @default.
- W2952011103 cites W2068942129 @default.
- W2952011103 cites W2069297302 @default.
- W2952011103 cites W2072237261 @default.
- W2952011103 cites W2095062440 @default.
- W2952011103 cites W2095310133 @default.
- W2952011103 cites W2097515434 @default.
- W2952011103 cites W2105898331 @default.
- W2952011103 cites W2115782706 @default.
- W2952011103 cites W2159044575 @default.
- W2952011103 cites W2170429490 @default.
- W2952011103 cites W2278489364 @default.
- W2952011103 cites W2385840111 @default.
- W2952011103 cites W2479406328 @default.
- W2952011103 cites W2504958700 @default.
- W2952011103 cites W2776671847 @default.
- W2952011103 cites W2794488170 @default.
- W2952011103 cites W3139479016 @default.
- W2952011103 cites W4362068852 @default.
- W2952011103 doi "https://doi.org/10.1016/j.fluid.2019.06.019" @default.
- W2952011103 hasPublicationYear "2019" @default.
- W2952011103 type Work @default.
- W2952011103 sameAs 2952011103 @default.
- W2952011103 citedByCount "2" @default.
- W2952011103 countsByYear W29520111032021 @default.
- W2952011103 countsByYear W29520111032022 @default.
- W2952011103 crossrefType "journal-article" @default.
- W2952011103 hasAuthorship W2952011103A5015464400 @default.
- W2952011103 hasAuthorship W2952011103A5039032609 @default.
- W2952011103 hasAuthorship W2952011103A5044409195 @default.
- W2952011103 hasAuthorship W2952011103A5070057968 @default.
- W2952011103 hasConcept C105569014 @default.
- W2952011103 hasConcept C121332964 @default.
- W2952011103 hasConcept C121864883 @default.
- W2952011103 hasConcept C134306372 @default.
- W2952011103 hasConcept C159985019 @default.
- W2952011103 hasConcept C178790620 @default.
- W2952011103 hasConcept C185592680 @default.
- W2952011103 hasConcept C192562407 @default.
- W2952011103 hasConcept C196806460 @default.
- W2952011103 hasConcept C204323151 @default.
- W2952011103 hasConcept C33923547 @default.
- W2952011103 hasConcept C44280652 @default.
- W2952011103 hasConcept C48372109 @default.
- W2952011103 hasConcept C48797263 @default.
- W2952011103 hasConcept C53810900 @default.
- W2952011103 hasConcept C57879066 @default.
- W2952011103 hasConcept C6648577 @default.
- W2952011103 hasConcept C70615421 @default.
- W2952011103 hasConcept C7772457 @default.
- W2952011103 hasConcept C8892853 @default.
- W2952011103 hasConcept C93779851 @default.
- W2952011103 hasConcept C94375191 @default.
- W2952011103 hasConcept C97355855 @default.
- W2952011103 hasConcept C97937538 @default.
- W2952011103 hasConceptScore W2952011103C105569014 @default.
- W2952011103 hasConceptScore W2952011103C121332964 @default.
- W2952011103 hasConceptScore W2952011103C121864883 @default.
- W2952011103 hasConceptScore W2952011103C134306372 @default.
- W2952011103 hasConceptScore W2952011103C159985019 @default.
- W2952011103 hasConceptScore W2952011103C178790620 @default.
- W2952011103 hasConceptScore W2952011103C185592680 @default.
- W2952011103 hasConceptScore W2952011103C192562407 @default.
- W2952011103 hasConceptScore W2952011103C196806460 @default.
- W2952011103 hasConceptScore W2952011103C204323151 @default.
- W2952011103 hasConceptScore W2952011103C33923547 @default.
- W2952011103 hasConceptScore W2952011103C44280652 @default.
- W2952011103 hasConceptScore W2952011103C48372109 @default.