𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Re-entrant corner flows of UCM fluids: The Cartesian stress basis

✍ Scribed by J.D. Evans


Publisher
Elsevier Science
Year
2008
Tongue
English
Weight
980 KB
Volume
150
Category
Article
ISSN
0377-0257

No coin nor oath required. For personal study only.

✦ 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.


πŸ“œ SIMILAR VOLUMES


Re-entrant corner flows of UCM fluids: T
✍ J.D. Evans πŸ“‚ Article πŸ“… 2008 πŸ› Elsevier Science 🌐 English βš– 763 KB

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 PTT fluids in
✍ J.D. Evans; D.N. Sibley πŸ“‚ Article πŸ“… 2008 πŸ› Elsevier Science 🌐 English βš– 427 KB

We consider the planar flow of Phan-Thien-Tanner (PTT) fluids around a re-entrant corner of angle Ο€/Ξ± where Ξ± ∈ [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

Re-entrant corner flow for PTT fluids in
✍ J.D. Evans; D.N. Sibley πŸ“‚ Article πŸ“… 2009 πŸ› Elsevier Science 🌐 English βš– 646 KB

We revisit the situation of steady planar flow of Phan-Thien-Tanner (PTT) fluids around re-entrant corners of angles /Λ›where 1/2 ≀ 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 -

The UCM limit of the PTT equations at a
✍ J.D. Evans; D.N. Sibley πŸ“‚ Article πŸ“… 2010 πŸ› Elsevier Science 🌐 English βš– 304 KB

We consider the Upper Convected Maxwell (UCM) limit of the Phan-Thien-Tanner (PTT) equations for steady planar flow around re-entrant corners. The PTT equations give the UCM equations in the limit of vanishing model parameter Γ„, this dimensionless parameter being associated with the quadratic stress