Gas-assisted non-Newtonian fluid displacement in circular tubes and noncircular channels

dc.contributor.authorKamisli, F
dc.contributor.authorRyan, ME
dc.date.accessioned2026-08-12T17:26:07Z
dc.date.issued2001
dc.departmentFırat Üniversitesi
dc.description.abstractThe motion of long bubbles into Newtonian and non-Newtonian fluids confined in horizontal circular tubes, rectangular channels, and square cross-sectional channels has been studied both theoretically and experimentally. Of particular interest is the determination of residual liquid film thickness on the walls. Isothermal experiments have been conducted to measure the displacement of the gas-liquid interface as a function of the applied pressure differential. The velocity of the interface and residual liquid film thickness have been determined for both Newtonian and non-Newtonian (shear thinning and viscoelastic) fluids. These experimental results are in good agreement with similar experimental studies conducted by other investigators. The experimental results indicate that the liquid film thickness of constant viscosity viscoelastic fluids (Boger fluids) deposited on the tube wall is thicker than that of comparable Newtonian fluids. A simple mathematical analysis was developed using a power-law model. The mathematical model successfully captures the gas-liquid dynamics for Newtonian and non-Newtonian fluid displacement in a tube and rectangular channel. The prediction of the liquid fraction deposited on the walls is in qualitative agreement with the experimental observations of previous investigators (Chem. Eng. Sci. 24 (1969) 471; A.I.Ch.E. 16 (1970) 925; Chem. Eng. Sci. 30 (1975) 379). The model gives similar results to a numerical solution (Polm. Eng. Sci. 35 (1995) 877) in which a constitutive equation containing a yield stress is used to model the non-Newtonian behavior. The model is used to determine the location and velocity of the advancing bubble front for the case of a power-law fluid. The results indicate that the gas-liquid interface advances more rapidly with decreasing values of the power-law index above a certain value of dimensionless time (t/t(b) approximate to 0.75). (C) 2001 Elsevier Science Ltd. All rights reserved.
dc.identifier.doi10.1016/S0009-2509(01)00136-1
dc.identifier.endpage4928
dc.identifier.issn0009-2509
dc.identifier.issue16
dc.identifier.scopus2-s2.0-0035860380
dc.identifier.scopusqualityQ1
dc.identifier.startpage4913
dc.identifier.urihttps://doi.org/10.1016/S0009-2509(01)00136-1
dc.identifier.urihttps://hdl.handle.net/11508/54694
dc.identifier.volume56
dc.identifier.wosWOS:000170930600016
dc.identifier.wosqualityQ2
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.language.isoen
dc.publisherPergamon-Elsevier Science Ltd
dc.relation.ispartofChemical Engineering Science
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.snmzKA_WoS_20260511
dc.subjecttwo-phase flow
dc.subjectgas-assisted flow
dc.subjectshear thinning fluid
dc.subjectviscoelastic fluid
dc.titleGas-assisted non-Newtonian fluid displacement in circular tubes and noncircular channels
dc.typeArticle

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