The flow rate of a steady flow of viscoelastic fluid under a constant axial pressure gradient in a toroidal pipe of circular cross-section is analytically solved with the White-Metzner constitutive equation by a perturbation method. It is examined how the shear thinning viscosity and elasticity affect the flow rate of the fluid at high shear-rate to which former analyses could not be applied.
The analysis shows that the characteristics of the flow in a curved pipe are determined not only by the Dean number but also by the non-dimensional value
We; /√<R> where
We; is the Weissenberg number and
R is the ratio of the toroidal radius to the pipe cross-sectional one. The results calculated for the ratio
fr; of the flow rate in a toroidal pipe to that in a straight pipe under the same axial pressure gradient at low Reynolds number are as follows:
(1) In the case of the Power law fluid in which
We; is zero,
fr; decreases with increment of the Reynolds number
Re; and with decrement of the viscosity index
n representing the shear thinning viscosity. Thus, the pipe resistance in a curved pipe is higher than that in a straight one.
(2) The larger
We; gives the larger
fr; and thus the smaller pipe resistance.
(3) Large
Re; and small
n give large increment of
fr; with increasing
We; .
(4) The effect of the elasticity index s, representing the shear thinning elasticity, on
fr; is insignificant unless
n is small.
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