Plane contraction flows of upper convected Maxwell and Phan-Thien–Tanner fluids as predicted by a finite-volume method

A finite-volume (FV) procedure is applied to the prediction of two-dimensional (2-D) laminar flow through a 4 : 1 planar contraction of upper convected Maxwell (UCM) and simplified Phan-Thien‐Tanner (SPTT) fluids. The method incorporates general coordinates, indirect addressing for easy mapping of complex domains, and is based on the collocated mesh arrangement. Calculations with the UCM model at a Reynolds number of 0.01 were carried out with three consecutively refined meshes which enabled the estimation of the accuracy of the predictions of the main vortex characteristics through Richardson’s extrapolation. Converged solutions with the first-order upwind differencing scheme for the convective terms were obtained up to at least Dea 8 in the finest mesh, but were limited to De 1, De 3 and De 5 for the fine, medium and coarse meshes, respectively, when using the second-order linear upwind scheme. The predicted flow patterns for increasing Deborah numbers with the UCM model resemble the well known lip vortex enhancement mechanism reported in the literature for constant-viscosity fluids in axisymmetric contractions and shear-thinning fluids in planar contraction, but very fine meshes were required in order to capture the described vortex activity. Predictions with the SPTT model also compared well with the behaviour reported in the literature. # 1999 Elsevier Science B.V. All rights reserved.

[1]  S. White,et al.  Flow visualization and birefringence studies on planar entry flow behavior of polymer melts , 1988 .

[2]  N. Phan-Thien,et al.  Three dimensional numerical simulations of viscoelastic flows through planar contractions , 1998 .

[3]  S. Richardson,et al.  Explicit numerical simulation of time-dependent viscoelastic flow problems by a finite element/finite volume method , 1994 .

[4]  Marcel Crochet,et al.  Hermitian Finite-elements for Calculating Viscoelastic Flow , 1986 .

[5]  D. V. Boger,et al.  Further observations of elastic effects in tubular entry flows , 1986 .

[6]  F. Pinho,et al.  Numerical simulation of non-linear elastic flows with a general collocated finite-volume method , 1998 .

[7]  K. Walters,et al.  Further remarks on the lip-vortex mechanism of vortex enhancement in planar-contraction flows , 1989 .

[8]  Marcel Crochet,et al.  Plane flow of a fluid of second grade through a contraction , 1976 .

[9]  S. Patankar Numerical Heat Transfer and Fluid Flow , 2018, Lecture Notes in Mechanical Engineering.

[10]  C. Rhie,et al.  Numerical Study of the Turbulent Flow Past an Airfoil with Trailing Edge Separation , 1983 .

[11]  Dionysis Assimacopoulos,et al.  A finite volume approach in the simulation of viscoelastic expansion flows , 1998 .

[12]  D. M. Binding,et al.  An approximate analysis for contraction and converging flows , 1988 .

[13]  R. Issa,et al.  NUMERICAL PREDICTION OF PHASE SEPARATION IN TWO-PHASE FLOW THROUGH T-JUNCTIONS , 1994 .

[14]  M. F. Webster,et al.  On the simulation of highly elastic complex flows , 1995 .

[15]  K. Walters,et al.  Long range memory effects in flows involving abrupt changes in geometry: Part 2: the expansion/contraction/expansion problem , 1977 .

[16]  R. Armstrong,et al.  Birefringence and laser-Doppler velocimetry (LDV) studies of viscoelastic flow through a planar contraction , 1994 .

[17]  D. V. Boger Viscoelastic Flows Through Contractions , 1987 .

[18]  Marcel Crochet,et al.  Flows of polymer solutions through contractions .1. Flows of polyacrylamide solutions through planar contractions , 1996 .

[19]  J. Song,et al.  Numerical simulation of viscoelastic flow through a sudden contraction using a type dependent difference method , 1987 .

[20]  J. Ferziger Numerical methods for engineering application , 1981 .

[21]  J. P. V. Doormaal,et al.  ENHANCEMENTS OF THE SIMPLE METHOD FOR PREDICTING INCOMPRESSIBLE FLUID FLOWS , 1984 .

[22]  M. F. Webster,et al.  A taylor-petrov-galerkin algorithm for viscoelastic flow , 1993 .

[23]  G. P Sasmal,et al.  A finite volume approach for calculation of viscoelastic flow through an abrupt axisymmetric contraction , 1995 .

[24]  R. Armstrong,et al.  Finite element methdos for calculation of steady, viscoelastic flow using constitutive equations with a Newtonian viscosity , 1990 .

[25]  R. Larson Constitutive equations for polymer melts and solutions , 1988 .

[26]  J. Yoo,et al.  A NUMERICAL STUDY OF THE PLANAR CONTRACTION FLOW OF A VISCOELASTIC FLUID USING THE SIMPLER ALGORITHM , 1991 .

[27]  M. F. Webster,et al.  Recovery and stress-splitting schemes for viscoelastic flows , 1998 .

[28]  B. Tremblay Visualization of the flow of low density polyethylene/polystyrene blends through a planar step contraction , 1994 .

[29]  R. Armstrong,et al.  Use of coupled birefringence and LDV studies of flow through a planar contraction to test constitutive equations for concentrated polymer solutions , 1995 .

[30]  N. Phan-Thien,et al.  Numerical investigations of Lagrangian unsteady extensional flows of viscoelastic fluids in 3-D rectangular ducts with sudden contractions , 1998 .

[31]  M. Crochet,et al.  A new mixed finite element for calculating viscoelastic flow , 1987 .

[32]  S. White,et al.  Numerical simulation studies of the planar entry flow of polymer melts , 1988 .

[33]  Joel H. Ferziger,et al.  Computational methods for fluid dynamics , 1996 .

[34]  K. Walters,et al.  Flow characteristics associated with abrupt changes in geometry in the case of highly elastic liquids , 1986 .

[35]  D. Joseph,et al.  Principles of non-Newtonian fluid mechanics , 1974 .