Slow steady fall of rigid bodies in a second-order fluid

We consider the steady, slow translational fall of a rigid body B in a second-order fluid, under the action of the force of gravity g. We find a general expression for the total force and torque acting on B . In particular, the force per unit area is always compressive, if the first normal stress co...

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Bibliographic Details
Published in:Journal of non-Newtonian fluid mechanics Vol. 90; no. 1; pp. 81 - 89
Main Author: Galdi, Giovanni P.
Format: Journal Article
Language:English
Published: Amsterdam Elsevier B.V 01-04-2000
Elsevier
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Summary:We consider the steady, slow translational fall of a rigid body B in a second-order fluid, under the action of the force of gravity g. We find a general expression for the total force and torque acting on B . In particular, the force per unit area is always compressive, if the first normal stress coefficient Ψ 1 is positive. We then specialize these formulas to the case when B is a prolate spheroid of eccentricity e, and show that, when 0 < e < 1, there are only two orientations of fall allowed, namely, when the major axis of B is either perpendicular or parallel to g. However, we show that if Ψ 1 >0, only this latter orientation is stable to small disorientations, in agreement with the recent experimental results of Joseph and coworkers.
ISSN:0377-0257
1873-2631
DOI:10.1016/S0377-0257(99)00045-2