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Thermo-fluid dynamics of the unsteady channel flow
Authors:Amilcare Pozzi  Renato Tognaccini
Institution:1. Faculty of Physics, West University of Timisoara, Bd. V. Parvan 4, 300223, Timisoara, Romania;2. HPC Center, West University of Timisoara, Bd. V. Parvan 4, 300223, Timisoara, Romania;1. University of Liege, Gembloux Agro-Bio Tech, Gembloux 5030, Belgium;2. von Karman Institute, Environmental and Applied Fluid Dynamics Department, Rhode-Saint-Genèse 1640, Belgium;1. Guangzhou Institute of Energy Conversion, Chinese Academy of Sciences, Guangzhou 510640, China;2. CAS Key Laboratory of Renewable Energy, Guangzhou 510640, China;3. Guangdong Provincial Key Laboratory of New and Renewable Energy Research and Development, Guangzhou 510640, China;4. University of Chinese Academy of Sciences, Beijing 100049, China;1. Department of Physics and Nanomed Labs, Università di Genova, Via Dodecaneso 33, 16146 Genova, Italy;2. In?titut Za Kovinske Materiale in Tehnologije, Lepi pot 11, 1000 Ljubljana, Slovenia;1. Department of Mathematics, Karnatak University, Pavate Nagar, Dharwad, 580003, India;2. Department of Computer Science (MCA), KLE Technological University, BVB Campus, Hubli, 580031, India
Abstract:We present an exact analytical representation of the unsteady thermo-fluid dynamic field arising in a two-dimensional channel with parallel walls for a fluid with constant properties. We assume that the axial pressure gradient is an arbitrary function of time that can be expanded in Taylor series; a particular case is the impulsive motion generated by a sudden jump to a constant value; for large time values the flow reaches the well-known steady Poiseuille solution. As boundary conditions for the dynamic field we consider fixed and moving walls (unsteady Couette flow). The assigned temperature on the walls can be an arbitrary function of time. We also consider the coupling of the energy and momentum equations (i.e. Eckert number different from zero). The solution is obtained by series with simple expressions of the coefficients in terms of the error functions. The fundamental physical parameters, such as shear stress, mass flow and heat flux at the wall are obtained in explicit analytical form and discussed by means of their diagrams.
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