Abstract
The vane is an
n
-bladed paddle which rotates with angular velocity
Ω
in a linear viscoelastic fluid. The blades, of zero thickness, are equally spaced around the axis
r
= 0, and extend from
r
= 0 to
r
=
a
. The problem is assumed two-dimensional. The stress and fluid velocity (or material displacements) are obtained by a Wiener–Hopf technique for the case of a no-slip boundary condition on the surface of the blades, and for the case of zero shear stress on the blades. The torque
M
(per unit length) required to rotate the vane in an incompressible newtonian fluid of viscosity
μ
may be approximated as
M
≈ 4π
μa
2
Ω
(1 –
n
–1
) to within 1% for the no-slip boundary condition; with the slip boundary condition the same expression is accurate to within 4%. Results are also given for the angular dependence and strength of the stress singularity at the tip of each blade.
Cited by
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