In this paper we study, by means of numerical simulation, planar elongational flow of concd., inertialess, non-Brownian rigid particle suspensions in a viscoelastic fluid. The simulation is 2D and follows the approach presented in our previous work [G. D'Avino, P.L. Maffettone, M.A. Hulsen, G.W.M. Peters, A numerical method for simulating concd. rigid particle suspensions in an elongational flow using a fixed grid, J. Comput. Phys. 226 (2007) 688-711]. A small computational domain is obtained by considering a three-layer domain. The innermost part is used to calc. the suspension response, the outermost is used to set the elongational flow boundary conditions far from the particles, and an intermediate region is mandatory to allow the developing of viscoelastic stress fields around the particle before entering the innermost layer. This scheme allows to achieve steady state (in a statistical sense). A time-independent fixed grid is used to avoid difficulties due to deforming meshes and remeshing of the domain. A fictitious domain has been implemented in order to easily manage the rigid-body motion. The particles are described by their boundaries only (rigid-ring description) and the rigid-body motion is imposed through Lagrange multipliers. A DEVSS-G/SUPG finite element formulation is implemented, and the log-conformation representation of the constitutive equation is used in order to improve the numerical stability of the method. The suspending liq. is treated as a Giesekus fluid. The bulk properties are detd. by using an averaging procedure. Bulk calcns. show that the extensional viscosity increases, with respect to the unfilled fluid, with the particle area fraction as well as with the Weissenberg no. The strain hardening parameter is predicted to decrease with increasing particle area fraction. The relative increase of the strain hardening parameter with increasing Weissenberg nos. is greatly reduced for larger particle area fraction. The predicted redn. of strain hardening agrees with exptl. evidence.
Numerical simulation of planar elongational flow of concentrated rigid particle suspensions in a viscoelastic fluid / D'Avino, Gaetano; Maffettone, PIER LUCA; M. A., Hulsen; G. W., M.. - In: JOURNAL OF NON-NEWTONIAN FLUID MECHANICS. - ISSN 0377-0257. - 150:2-3(2008), pp. 65-79. [10.1016/j.jnnfm.2007.10.001]
Numerical simulation of planar elongational flow of concentrated rigid particle suspensions in a viscoelastic fluid
D'AVINO, GAETANO;MAFFETTONE, PIER LUCA;
2008
Abstract
In this paper we study, by means of numerical simulation, planar elongational flow of concd., inertialess, non-Brownian rigid particle suspensions in a viscoelastic fluid. The simulation is 2D and follows the approach presented in our previous work [G. D'Avino, P.L. Maffettone, M.A. Hulsen, G.W.M. Peters, A numerical method for simulating concd. rigid particle suspensions in an elongational flow using a fixed grid, J. Comput. Phys. 226 (2007) 688-711]. A small computational domain is obtained by considering a three-layer domain. The innermost part is used to calc. the suspension response, the outermost is used to set the elongational flow boundary conditions far from the particles, and an intermediate region is mandatory to allow the developing of viscoelastic stress fields around the particle before entering the innermost layer. This scheme allows to achieve steady state (in a statistical sense). A time-independent fixed grid is used to avoid difficulties due to deforming meshes and remeshing of the domain. A fictitious domain has been implemented in order to easily manage the rigid-body motion. The particles are described by their boundaries only (rigid-ring description) and the rigid-body motion is imposed through Lagrange multipliers. A DEVSS-G/SUPG finite element formulation is implemented, and the log-conformation representation of the constitutive equation is used in order to improve the numerical stability of the method. The suspending liq. is treated as a Giesekus fluid. The bulk properties are detd. by using an averaging procedure. Bulk calcns. show that the extensional viscosity increases, with respect to the unfilled fluid, with the particle area fraction as well as with the Weissenberg no. The strain hardening parameter is predicted to decrease with increasing particle area fraction. The relative increase of the strain hardening parameter with increasing Weissenberg nos. is greatly reduced for larger particle area fraction. The predicted redn. of strain hardening agrees with exptl. evidence.File | Dimensione | Formato | |
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