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Analysis of compressible potential flow over aerofoils using the dual reciprocity method

Published online by Cambridge University Press:  27 January 2016

A. V. G. Cavalieri
Affiliation:
Instituto Tecnológico de Aeronáutica, São José dos Campos, São Paulo, Brazil
P. A. O. Soviero*
Affiliation:
Instituto Tecnológico de Aeronáutica, São José dos Campos, São Paulo, Brazil

Abstract

The use of the linearised potential model for the analysis of compressible flows is quite widespread, and provides good results for subsonic and supersonic flows. However, the calculation of aerofoils and wings subject to transonic flows requires a non-linear model, such as the transonic small-disturbance (TSD) potential equation. The solution of the problem by a singularity distribution requires singularities over the field, as well as panels on the boundary, characterising the procedure known as field panel method. The present work shows results of calculations of the transonic small-disturbance potential equation for flows without shock waves using the dual reciprocity method (DRM), which permits calculation of integrals only at the boundary of the problem, without the need of field distributions. This approach, compared to the field panel methods, takes considerably less computer time, and shows a significant improvement when compared to results of linear theory without much additional computer time, making this technique adequate to design phases of aircraft. Pressure distribution results show good agreement with other methods found in litterature. The low computational cost of the present method allows us to perform parametric tests and explore the effects of thickness and Mach number on the lift and pitching moment coefficients. A discussion of the physical effect of these parameters on the problem is presented, and the thickness of the aerofoil is shown to increase the lift and change the position of the aerodynamic centre. However, this non-linear effect depends on the precise shape of the thickness distribution.

Type
Research Article
Copyright
Copyright © Royal Aeronautical Society 2012 

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References

1. Hess, J. and Smith, A.M.O. Calculation of potential flow about arbitrary bodies, Progress in Aerospace Sciences, 1967, 8, pp 1138.Google Scholar
2. Spreiter, J.R. and Alksne, A. Theoretical prediction of pressure distributions on nonlifting airfoils at high subsonic speeds, 1954, Tech Rep TR-1217, National Advisory Committee for Aeronautics.Google Scholar
3. Nixon, D. Transonic flow around symmetric aerofoils at zero incidence, J Aircr, 1974, 11, pp 122124.Google Scholar
4. Ribeiro, R.S. and Soviero, P.A.O. Calculation of transonic flow about airfoils by a field panel method, Boundary element techniques: Applications in fluid flow and computational aspects, 1987.Google Scholar
5. Houwink, R. and Van der Vooren, J. Improved version of LTRAN2 for unsteady transonic flow computations, AIAA J, 1980, 18, pp 10081010.Google Scholar
6. Morino, L., Gennaretti, M., Iemma, U. and Salvatore, F. Aerodynamics and aeroacoustics of wings and rotors via BEM-unsteady, transonic, and viscous effects, Computational Mechanics, 1998, 21, (4), pp. 265275.Google Scholar
7. Gebhardt, L., Fokin, D., Lutz, T. and Wagner, S. An implicit-explicit Dirichlet-based field panel method for transonic aircraf design, 2002, 20th AIAA Applied Aerodynamics Conference, American Institute of Aeronautics and Astronautics.Google Scholar
8. Holst, T.L. Transonic flow computations using nonlinear potential methods, Progress in Aerospace Sciences, 2000, 36, (1), pp 161.Google Scholar
9. Partridge, P.W., Brebbia, C.A. and Wrobel, L.C. The dual reciprocity boundary element method, 1992, Computational Mechanics Publications.Google Scholar
10. Theurer, R. and Wagner, S. Inviscid transonic flow computation using the dual reciprocity method, Boundary Element Technology XI, 1996, pp 1322.Google Scholar
11. Uhl, B., Ostertag, J., Guidati, G. and Wagner, S. Application of the dual-reciprocity method to three-dimensional compressible flows governed by the full-potential equation, 1999, 37th AIAA Aerospace Sciences Meeting and Exhibit, Reno, NV, American Institute of Aeronautics and Astronautics.Google Scholar
12. Hunt, B. The panel method for subsonic aerodynamic flow: A survey of mathematical formulations and numerical models with an outline of the new British aerospace scheme, Computational Fluid Dyn, 1978, 1, VKI, Von Karman Inst for Fluid Dyn.Google Scholar
13. Cavalieri, A.V.G. Calculation of Transonic Flow over Airfoils using the Dual Reciprocity Method (in Portuguese), 2006, Master thesis.Google Scholar
14. Schlichting, H. and Truckenbrodt, E. Aerodynamics of the Airplane, 1979, McGraw-Hill.Google Scholar
15. Ribeiro, R.S. Analysis of Transonic Flow by the Method of Singularities (in Portuguese), 1987, Master thesis.Google Scholar
16. Knechtel, E.D. Experimental investigation at transonic speeds of pressure distributions over wedge and circular-arc airfoil sections and evaluation of perforated-wall, 1959, Tech Rep TN-D-15, National Aeronautics and Space Administration.Google Scholar
17. Harris, C.D. Two-dimensional aerodynamic characteristics of the NACA 0012 airfoil in the Langley 8 foot transonic pressure tunnel, 1981, Tech Rep TM-81927, National Advisory Committee for Aeronautics.Google Scholar
18. Abbott, I.H. and Von Doenhoff, A.E. Theory of wing sections: including a summary of airfoil data, 1959, Dover Publications.Google Scholar