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On the skin friction coefficient in viscoelastic wall-bounded flows
Institution:1. Department of Mathematics, University of the Aegean, Karlovassi 83200, Samos, Greece;2. Department of Chemical & Biomolecular Engineering, University of Delaware, Newark, DE 19716, USA;1. Jiangsu Vocational Institute of Architectural Technology, Xuzhou 221116, Jiangsu, China;2. Xuzhou Intelligent Machine Vision Engineering and Technology Center, Xuzhou 221116, Jiangsu, China;3. Department of Mathematics, College of Science, King Saud University, Riyadh 11451, Saudi Arabia;4. Department of Science and Environmental Studies, Lakehead University, Thunder Bay, ON P7B 5E1, Canada;5. Department of Mathematical and Computer Modeling, Al-Farabi Kazakh National University, Almaty, Kazakhstan;6. Department of Mathematical and Computer Modeling, Kazakh-British Technical University, Almaty, Kazakhstan;7. Future Technology Research Center, National Yunlin University of Science and Technology, 123 University Road, Section 3, Douliou, Yunlin 64002, Taiwan, ROC;1. National Institute for Mathematical Sciences, Daejeon 34047, Republic of Korea;2. Department of Mathematics, Ewha Woman''s University, Seoul 03760, Republic of Korea
Abstract:Analysis of the skin friction coefficient for wall bounded viscoelastic flows is performed by utilizing available direct numerical simulation (DNS) results for viscoelastic turbulent channel flow. The Oldroyd-B, FENE-P and Giesekus constitutive models are used. First, we analyze the friction coefficient in viscous, viscoelastic and inertial stress contributions, as these arise from suitable momentum balances, for the flow in channels and pipes. Following Fukagata et al. (Phys. Fluids, 14, p. L73, 2002) and Yu et al. (Int. J. Heat. Fluid Flow, 25, p. 961, 2004) these three contributions are evaluated averaging available numerical results, and presented for selected values of flow and rheological parameters. Second, based on DNS results, we develop a universal function for the relative drag reduction as a function of the friction Weissenberg number. This leads to a closed-form approximate expression for the inverse of the square root of the skin friction coefficient for viscoelastic turbulent pipe flow as a function of the friction Reynolds number involving two primary material parameters, and a secondary one which also depends on the flow. The primary parameters are the zero shear-rate elasticity number, El0, and the limiting value for the drag reduction at high Weissenberg number, LDR, while the secondary one is the relative wall viscosity, μw. The predictions reproduce both types A and B of drag reduction, as first introduced by Virk (Nature, 253, p. 109, 1975), corresponding to partially and fully extended polymer molecules, respectively. Comparison of the results for the skin friction coefficient against experimental data shows good agreement for low and moderate drag reduction which is the region covered by the simulations.
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