53rd AIAA Aerospace Sciences Meeting 2015
DOI: 10.2514/6.2015-1722
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Drag minimization of an isolated airfoil in transonic inviscid flow by means of genetic algorithms

Abstract: The paper deals with the shape optimization of an isolated airfoil to minimize the drag when operating in a transonic inviscid flow with some prescribed constraints. A nondominated Sorting Genetic Algorithm is used to solve the optimization problem. Other numerical ingredients of the optimization loop are given by the Class/Shape function Transformation used for the parameterization of the airfoil shape and a finite-volume Computational Fluid Dynamics solver of the Euler equations.

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Cited by 6 publications
(4 citation statements)
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“…This case has previously been investigated with a variety of different parameterisation methods: Bèzier Curves [1,2]; B-Splines [3,4,5,6,7]; NURBS [8]; Class/Shape Transformations (CSTs) [9]; Hicks-Henne bump functions [10]; Bèzier Surface FFD [11]; PARSEC [12]; Radial basis function domain element (RBF-DE) deformation [13,14] and Singular Value Decompositions (SVD) [14,15]. Due to the large range of factors influencing the results it is difficult to isolate contribution of the parameterisation method from these previous studies.…”
Section: Introductionmentioning
confidence: 99%
“…This case has previously been investigated with a variety of different parameterisation methods: Bèzier Curves [1,2]; B-Splines [3,4,5,6,7]; NURBS [8]; Class/Shape Transformations (CSTs) [9]; Hicks-Henne bump functions [10]; Bèzier Surface FFD [11]; PARSEC [12]; Radial basis function domain element (RBF-DE) deformation [13,14] and Singular Value Decompositions (SVD) [14,15]. Due to the large range of factors influencing the results it is difficult to isolate contribution of the parameterisation method from these previous studies.…”
Section: Introductionmentioning
confidence: 99%
“…The wing geometry has an initial volume of V = 0.24 cubed reference units and a reference area of S = 3.0 squared reference units. The flow analysis is performed at a Reynolds number of 20⇥10 6 and at both Mach 0.78 and Mach 0.85. Despite the fact that the wing chords are free to change, the final geometries are tapered such that the overall mean aerodynamic chord is close to one, meaning that the initial Reynolds number is still valid at the end of optimization.…”
Section: Optimization Problemmentioning
confidence: 99%
“…Even with advanced techniques to balance the exploration and exploitation of the design space [4][5][6][7][8], this can still make optimization intractable for complex geometries.…”
Section: Introductionmentioning
confidence: 99%