1956 Volume 11 Issue 6 Pages 690-701
The steady slow motion of a viscous fluid past two parallel circular cylinders C1, C2 of arbitrary radii is discussed on the basis of Oseen’s linearized equations of motion, confining ourselves to the case when their axes are perpendicular to a uniform flow. The forces acting on the cylinder C1 are calculated to the first approximation.
By performing detailed numerical calculations, a discussion is made on the manner in which the forces acting on the cylinder C1 is modified by the presence of the other cylinder C2.
It is thus found that, as the radius of the cylinder C2 increases, the drag on the cylinder C1 decreases, while the lift increases. It is also found that the cylinder C1 experiences smaller drag when the two cylinders are in tandem orientation than when they are placed side by side in a uniform stream. Especially, when the cylinder C1 is situated behind the cylinder C2, it experiences smaller drag than when it is situated in front of C2.
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