Application of Modified 4th Order Runge Kutta-TVD Scheme for the Flow Past through Symmetrical Model

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Computational fluid dynamics (CFD) is a well known tool to solve the fluid flow problems. In CFD analysis, the models use various types of Partial Differential Equation (PDE). The most common is hyperbolic equation. In order to solve the equation, high-order scheme is very reasonable to be applied due to the accuracy of result. So that, this study use modified Runge Kutta with Total Variation Diminishing (TVD) scheme and the model is half body airfoil (symmetrical airfoil NACA 0012). Firstly, parametric study over the size of suitable flow domain was carried out. If the length of airfoil chord is denoted by c, investigation effects on the size of flow domain is carried over the flow domain in x-direction which is 5c while in y-direction is 6c. Another two size flow domains had been used in this study are 5c×3c and 9c×3c respectively. The result shows a strong influence to the flow field solution occurred if the distance between airfoil surfaces to the outer boundary is relatively small. Through this parametric study, it had been suggested that the best way to solve the aerodynamics problem for the flow past through symmetrical airfoil by using the size of flow domain is 5c×6c. Using the same size of flow domain, it had been found that the developed computer code able to produce the result in a good agreement with ANSYS CFD-FLUENT software.

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181-185

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April 2013

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© 2013 Trans Tech Publications Ltd. All Rights Reserved

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[1] T.J. Chung, Computational Fluid Dynamics, 2nd ed., Cambridge University Press, New York, (2002).

Google Scholar

[2] H. Lomax & T.H. Pulliam, Fundamentals of Computational Fluid Dynamics, University of Toronto, Canada, (1999).

Google Scholar

[3] R. M. Mohan and P. Moin, Direct simulations of turbulent flow using finite-difference schemes, Journal of Computational Physics. 96 (1991) 15-53.

DOI: 10.1016/0021-9991(91)90264-l

Google Scholar

[4] J.C. Tannehill, D.A. Anderson & R.H. Pletcher, Computational Fluid Mechanics and Heat Transfer, 2nd ed., Taylor & Francis, United State of America, (1997).

Google Scholar

[5] B. Gustafsson & P. Olsson, Fourth-order difference methods for hyperbolic IVBs, Journal of Computational Physics. 117(1995) 300-317.

DOI: 10.1006/jcph.1995.1068

Google Scholar

[6] J.M. Corberan & M.L. Gascon, TVD scheme for the calculation of flow in pipes of variable cross-section, Mathl. Comput. Modelling. 21(1995) 85-92.

DOI: 10.1016/0895-7177(94)00216-b

Google Scholar

[7] J. Wang, Y. He & H. Ni, Two-Dimensional free surface in branch channels by a finite-volume TVD scheme. 26(2003) 623-633.

DOI: 10.1016/s0309-1708(03)00035-6

Google Scholar

[8] M. Bernardini & S. Pirozzoli, A general strategy for the optimization of Runge-Kutta scheme for wave propagation phenomena, Journal pf computational Physics. 228(2009) 4182-4199.

DOI: 10.1016/j.jcp.2009.02.032

Google Scholar

[9] K.S. Ravichandran, Higher order KFVS algorithms using compact upwind difference operators, Journal of Computational Physics. 130(1997) 161-173.

DOI: 10.1006/jcph.1996.5561

Google Scholar

[10] K.A. Hoffmann & S.T. Chiang, Computational Fluid Dynamics Volume II, 4th ed., www. EESbooks. com, USA, (2002).

Google Scholar

[11] T.J. Poinsot and S.K. Lelef, Boundary conditions for direct simulations of compressible viscous flows, Journal of Computational Physics. 101(1992) 104-129.

DOI: 10.1016/0021-9991(92)90046-2

Google Scholar