We consider stagnation point flow away from a wall for creeping flow of dilute polymer solutions. For a simplified flow geometry, we explicitly show that a narrow region of strong polymer extension (a birefringent strand) forms downstream of the stagnation point in the UCM model and extensions, like
Viscoelastic stresses in the stagnation flow of a dilute polymer solution
โ Scribed by Robert A. Van Gorder; K. Vajravelu; F. Talay Akyildiz
- Publisher
- Elsevier Science
- Year
- 2009
- Tongue
- English
- Weight
- 843 KB
- Volume
- 161
- Category
- Article
- ISSN
- 0377-0257
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โฆ Synopsis
In this paper, we consider viscoelastic stresses T 11 , T 12 and T 22 arising in the stagnation flow of a dilute polymer solution; in particular, we consider an upper convected Maxwell (UCM) fluid. We present exact solutions to the coupled partial differential equations describing the viscoelastic stresses and deduce the results for the stress T 22 of Becherer et al. [P. Becherer, A.N. Morozov, W. van Saarloos, Scaling of singular structures in extensional flow of dilute polymer solutions, J. Non-Newtonian Fluid Mech. 153 (2008) 183-190]. As we considered the viscoelastic stresses over two spatial variables, we are able to study the effect of variable boundary data at the inflow. As such, our results are applicable to a wider range of fluid flow problems.
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