Influence of flow confinement on the drag force on a static cylinder
Phys. Fluids 21, 103604 (2009); doi:10.1063/1.3253324
Published 30 October 2009
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The influence of confinement on the drag force F on a static cylinder in a viscous flow inside a rectangular slit of aperture h0 has been investigated from experimental measurements and numerical simulations. At low enough Reynolds numbers, F varies linearly with the mean velocity and the viscosity, allowing for the precise determination of drag coefficients 
and 
corresponding, respectively, to a mean flow parallel and perpendicular to the cylinder length L. In the parallel configuration, the variation in 
with the normalized diameter
=d/h0 of the cylinder is close to that for a two-dimensional (2D) flow invariant in the direction of the cylinder axis and does not diverge when
=1. The variation in 
with the distance from the midplane of the model reflects the parabolic Poiseuille profile between the plates for 
1 while it remains almost constant for
~1. In the perpendicular configuration, the value of 
is close to that corresponding to a 2D system only if 
1 and/or if the clearance between the ends of the cylinder and the side walls is very small: in that latter case, 
diverges as 
1 due to the blockage of the flow. In other cases, the side flow between the ends of the cylinder and the side walls plays an important part to reduce 
: a full three-dimensional description of the flow is needed to account for these effects.
©2009 American Institute of Physics

and 
corresponding, respectively, to a mean flow parallel and perpendicular to the cylinder length L. In the parallel configuration, the variation in 
with the normalized diameter
=d/h0 of the cylinder is close to that for a two-dimensional (2D) flow invariant in the direction of the cylinder axis and does not diverge when
=1. The variation in 
with the distance from the midplane of the model reflects the parabolic Poiseuille profile between the plates for 
1 while it remains almost constant for
~1. In the perpendicular configuration, the value of 
is close to that corresponding to a 2D system only if 
1 and/or if the clearance between the ends of the cylinder and the side walls is very small: in that latter case, 
diverges as 
1 due to the blockage of the flow. In other cases, the side flow between the ends of the cylinder and the side walls plays an important part to reduce 
: a full three-dimensional description of the flow is needed to account for these effects.
©2009 American Institute of Physics
| History: | Received 23 April 2009; accepted 18 September 2009; published 30 October 2009 |
| Permalink: |
http://link.aip.org/link/?PHFLE6/21/103604/1 |
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