Flow of fluid of non-uniform viscosity in converging and diverging channels

It is shown that the well-known Jeffery–Hamel solution of the Navier–Stokes equations admits generalization to the case in which the viscosity μ and density ρ are arbitrary functions of the angular co-ordinate θ. When |Rα| [Lt ] 1, where R is the Reynolds number and 2α the angle of divergence of the...

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Bibliographic Details
Published inJournal of fluid mechanics Vol. 117; pp. 283 - 304
Main Authors Hooper, Alison, Duffy, B. R., Moffatt, H. K.
Format Journal Article
LanguageEnglish
Published Cambridge, UK Cambridge University Press 01.04.1982
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ISSN0022-1120
1469-7645
DOI10.1017/S0022112082001633

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Summary:It is shown that the well-known Jeffery–Hamel solution of the Navier–Stokes equations admits generalization to the case in which the viscosity μ and density ρ are arbitrary functions of the angular co-ordinate θ. When |Rα| [Lt ] 1, where R is the Reynolds number and 2α the angle of divergence of the planes, lubrication theory is applicable; this limit is first treated in the context of flow in a channel of slowly varying width. The Jeffery–Hamel problem proper is treated in §§ 3–6, and the effect of varying the viscosity ratio λ in a two-fluid situation is studied. In § 5, results already familiar in the single-fluid context are recapitulated and reformulated in a manner that admits immediate adaptation to the two-fluid situation, and in § 6 it is shown that the singlefluid limit (λ → 1) is in a certain sense degenerate. The necessarily discontinuous behaviour of the velocity profile as the Reynolds number (based on volume flux) increases is elucidated. Finally, in § 7, some comments are made about the realizability of these flows and about instabilities to which they may be subject.
Bibliography:istex:CA7A9B46E728B0FDDFA37AB12F011B92083C3589
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PII:S0022112082001633
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ISSN:0022-1120
1469-7645
DOI:10.1017/S0022112082001633