This paper continues the description of a two parameter family of solutions for the local asymptotic behaviour of UCM fluids at re-entrant corners. Here, the natural stress basis is used to re-derive the equations in the core flow and boundary layers, with full description of the scalings and matchi
Re-entrant corner flows of UCM fluids: The Cartesian stress basis
β Scribed by J.D. Evans
- Publisher
- Elsevier Science
- Year
- 2008
- Tongue
- English
- Weight
- 980 KB
- Volume
- 150
- Category
- Article
- ISSN
- 0377-0257
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β¦ Synopsis
For a given re-entrant corner geometry, we describe a two parameter family of solutions for the local asymptotic behaviour of the flow and stress fields of UCM fluids. The two parameters used are the coefficients of the upstream wall shear rate and pressure gradient. In describing this parametric solution, the relationship between the Cartesian and natural stress basis is explained, reconciling these two equivalent formulations for the problem. The asymptotic solution structure investigated here comprises an outer (core) region together with inner regions (single wall boundary layers) located at the upstream and downstream walls. It is implicitly assumed that there are no regions of recirculation at the upstream wall, i.e. we consider flow in the absence of a lip vortex. The essential feature of the analysis is a full description of the matching between the outer and inner regions in both the Cartesian and natural stress bases, as well as the derivation of numerical estimates of important solution parameters such as the coefficients of the stream function and extra-stresses in the outer (core flow) region together with the downstream wall shear rate. This work is divided into two papers, the first one describing the solution structure in the Cartesian stress basis for the core and upstream boundary layer, and the second paper using the natural stress basis which allows the downstream boundary layer solution to be linked through the core to the upstream boundary layer solution. It is the latter formulation of this problem which allows a complete solution description.
π SIMILAR VOLUMES
We consider the planar flow of Phan-Thien-Tanner (PTT) fluids around a re-entrant corner of angle Ο/Ξ± where Ξ± β [1/2, 1). The model is considered in the absence of a solvent viscosity and the flow situation assumes complete flow around the corner with the absence of a lip votex. The local asymptotic
We revisit the situation of steady planar flow of Phan-Thien-Tanner (PTT) fluids around re-entrant corners of angles /Λwhere 1/2 β€ Λ< 1. The model is considered in the absence of a solvent viscosity, under which a class of self-similar solutions has been identified with stress singularities of O(r -
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