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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Published in: | Journal of non-Newtonian fluid mechanics Vol. 90; no. 1; pp. 81 - 89 |
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Main Author: | |
Format: | Journal Article |
Language: | English |
Published: |
Amsterdam
Elsevier B.V
01-04-2000
Elsevier |
Subjects: | |
Online Access: | Get full text |
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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. |
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ISSN: | 0377-0257 1873-2631 |
DOI: | 10.1016/S0377-0257(99)00045-2 |