1969
DOI: 10.1002/cjce.5450470318
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Bubble drag and mass transfer in non‐newtonian fluids: Creeping flow with power‐law fluids

Abstract: The drag and mass‐transfer characteristics of a gas bubble moving in power‐law non‐Newtonian fluids are examined analytically in terms of the rheological properties of the system. An approximate solution for the case of creeping flow around circulating bubbles shows that the mass‐transfer coefficient is enhanced for pseudoplastics and depressed for dilatants compared to the situation for Newtonian fluids. Some preliminary experimental results in support of the analysis are presented.

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Cited by 89 publications
(67 citation statements)
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“…By introducing these assumptions we have the linearized equations of motion. Following the derivation for a bubble in power-law fluids [18], we finally have an expression FD = 4zr (32"2) (n-l)/2 (13 + 4n -8n 2) (2n+l) (n+2) tloUooR. (15) This equation reduces to Co _ (3),2)(n_1)/2 (13 + 4n -8n 2)…”
Section: ~P=(l+22h/2)(n-1)/2[{1 ~mentioning
confidence: 99%
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“…By introducing these assumptions we have the linearized equations of motion. Following the derivation for a bubble in power-law fluids [18], we finally have an expression FD = 4zr (32"2) (n-l)/2 (13 + 4n -8n 2) (2n+l) (n+2) tloUooR. (15) This equation reduces to Co _ (3),2)(n_1)/2 (13 + 4n -8n 2)…”
Section: ~P=(l+22h/2)(n-1)/2[{1 ~mentioning
confidence: 99%
“…It will be assumed that the term H* can be approximately evaluated by using Newtonian flow solution as well as the analytical of Hirose and Moo-Young's [18] for bubbles in a power-law fluid and that the elasticity is strong (2* is large). By introducing these assumptions we have the linearized equations of motion.…”
Section: ~P=(l+22h/2)(n-1)/2[{1 ~mentioning
confidence: 99%
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“…Then, the power law non-Newtonian fluid model was used in the bubble drag and mass transfer problem [7]. D'Alessio and Pascal [8] presented a research for steady two-dimensional flow of power law fluid past a non-rotating circular cylinder.…”
Section: Introductionmentioning
confidence: 99%
“…The axial part of the solution using B. C. (7) is given by «&<(£) = «"* (12) and the radial part <fi(p) is given by *-&-+M(! -pn+1) =°d p (13) Eq.…”
Section: Introductionmentioning
confidence: 99%