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On bubble rising in a Hele–Shaw cell filled with a non-Newtonian fluid

Published online by Cambridge University Press:  01 September 2004

A. N. ALEXANDROU
Affiliation:
Department of Mechanical and Manufacturing Engineering, University of Cyprus, Nicosia, Cyprus
V. M. ENTOV
Affiliation:
Institute for Problems in Mechanics, Russian Academy of Science, 101-1, pr. Vernadskogo, Moscow, 119526, Russia email: entov@ipmnet.ru
S. S. KOLGANOV
Affiliation:
Russian Gubkin State Oil and Gas University, 65, Leninsky pr., Moscow, 117917, Russia
N. V. KOLGANOVA
Affiliation:
Russian Gubkin State Oil and Gas University, 65, Leninsky pr., Moscow, 117917, Russia

Abstract

The problem of a bubble rising due to buoyancy in a Hele–Shaw cell filled with a viscous fluid is a classical free-boundary problem first posed and solved by Saffman & Taylor [11]. In fact, due to linearity of the flow equations the problem is reduced to that of a bubble transported by uniform fluid flow. Saffman and Taylor provided explicit expressions for the bubble shape. Steady propagation of bubbles and fingers in a Hele–Shaw cell filled with a nonlinearly-viscous fluid was studied by Alexandrou & Entov [1]. In Alexandrou & Entov [1], it was shown that for a nonlinearly viscous fluid the problem of a rising bubble cannot be reduced to that of a steadily transported bubble, and should be treated separately. This note presents a solution of the problem following the general framework suggested in Alexandrou & Entov [1]. The hodograph transform is used in combination with finite-difference and collocation techniques to solve the problem. Results are presented for the cases of a Bingham and power-law fluids.

Type
Papers
Copyright
2004 Cambridge University Press

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