Inverse Problems in Engineering Mechanics 1998
DOI: 10.1016/b978-008043319-6/50049-2
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Fourier series solution for inverse design of aerodynamic shapes

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Cited by 7 publications
(5 citation statements)
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“…The MGM procedure was incorporated into a multigrid Navier-Stokes airfoil analysis method in [15]. Dulikravich & Baker [16] formulated a Fourier series solution of the MGM equation. The MGM technique was applied in [17] for the inverse design of vertical axis wind turbine blades with constant thickness, which represents a geometry substantially different from those described by airfoils.…”
Section: Introductionmentioning
confidence: 99%
“…The MGM procedure was incorporated into a multigrid Navier-Stokes airfoil analysis method in [15]. Dulikravich & Baker [16] formulated a Fourier series solution of the MGM equation. The MGM technique was applied in [17] for the inverse design of vertical axis wind turbine blades with constant thickness, which represents a geometry substantially different from those described by airfoils.…”
Section: Introductionmentioning
confidence: 99%
“…This is the major disadvantage of the method as the success of inverse design depends on the specification of these arbitrary constants. For airfoil design the amount of β 1 =1.2, β 2 =0, β 3 =0.4 was considered which are the same values which was proposed by Dulikravich and Baker [11].…”
Section: Target Calculatedmentioning
confidence: 99%
“…The airfoil surface is treated as elastic membrane, which is modified based on the differences between target and calculated pressure coefficient. The airfoil modifying algorithm is based on the method of Dulikravich and Baker [11] who suggested the following linear partial differential equations can be used as a residual corrector to modify the top and bottom contour of the blade respectively: (7) and equation (8), s is the airfoil contour following coordinate, L E is the lower airfoil contour length, L is the total airfoil counter length and ∆y top and ∆y bottom are the blade normal displacement at the top and bottom counter of the airfoil respectively. β 1 , β 2 , β 3 in equation (7) and equation (8) are user specified coefficients while ∆Cp is the local differences between the target and computed surface pressure coefficient i.e.…”
Section: Airfoil Modifying Algorithmmentioning
confidence: 99%
“…However, when using non-linear flow-field analysis such as Navier-Stokes solvers, this iterative inverse shape design method converges slowly. A semi-analytical method for integration of such differential equations has been developed that is based on Fourier series and converges much faster [21][22][23]. This formulation will be explained for the case of inverse shape design of an isolated three-dimensional airplane wing at arbitrary flight speed.…”
Section: Elastic Membrane Motion Concept For Inverse Determination Ofmentioning
confidence: 99%
“…Notice that coordinate directions s and t are not necessarily orthogonal to each other. Evolution model of the top surface of the wing can then be assumed to be of the form [21][22][23] (2)…”
Section: Elastic Membrane Motion Concept For Inverse Determination Ofmentioning
confidence: 99%