2018
DOI: 10.3390/aerospace5030092
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Unsteady Lifting Line Theory Using the Wagner Function for the Aerodynamic and Aeroelastic Modeling of 3D Wings

Abstract: A method is presented to model the incompressible, attached, unsteady lift and pitching moment acting on a thin three-dimensional wing in the time domain. The model is based on the combination of Wagner theory and lifting line theory through the unsteady Kutta–Joukowski theorem. The results are a set of closed-form linear ordinary differential equations that can be solved analytically or using a Runge–Kutta–Fehlberg algorithm. The method is validated against numerical predictions from an unsteady vortex lattic… Show more

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Cited by 27 publications
(24 citation statements)
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“…Since it is assumed that 2s c, and that changes in the flow happen on the span length-scale, the problem can be considered as 2D. The problem consists of a symmetric airfoil at a certain spanwise section undergoing small-amplitude pitch and plunge oscillations, h(y, t) = h * 0 (y)c(y)e iωt α(y, t) = α 0 (y)e i(ωt+ψ) (7) where h * 0 is plunge amplitude per unit chord, α 0 is pitch amplitude, ψ is the phase between plunge and pitch, and ω is the frequency of oscillation typically expressed as a chordwise or spanwise reduced frequency Figure 2 shows this problem, for which the solution is given by Theodorsen [60]. The results are expressed here in terms of a general unsteady thin-airfoil theory [36,52] which allows easy modification of the approach for various wing geometries and kinematics.…”
Section: The Inner Solutionmentioning
confidence: 99%
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“…Since it is assumed that 2s c, and that changes in the flow happen on the span length-scale, the problem can be considered as 2D. The problem consists of a symmetric airfoil at a certain spanwise section undergoing small-amplitude pitch and plunge oscillations, h(y, t) = h * 0 (y)c(y)e iωt α(y, t) = α 0 (y)e i(ωt+ψ) (7) where h * 0 is plunge amplitude per unit chord, α 0 is pitch amplitude, ψ is the phase between plunge and pitch, and ω is the frequency of oscillation typically expressed as a chordwise or spanwise reduced frequency Figure 2 shows this problem, for which the solution is given by Theodorsen [60]. The results are expressed here in terms of a general unsteady thin-airfoil theory [36,52] which allows easy modification of the approach for various wing geometries and kinematics.…”
Section: The Inner Solutionmentioning
confidence: 99%
“…The first unsteady finite wing analysis in the time domain is due to Jones [35], although it is only applicable to elliptic planforms. A time-domain ULLT is presented by Boutet and Dimitriatis [7] using an inner solution based on Wagner's method [67], and a pseudosteady assumption. Ramesh et al [54] introduce a lifting-line theory for a geometrically nonlinear inner solution, again using a pseudosteady assumption.…”
Section: Introductionmentioning
confidence: 99%
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“…Another method is based on the computational aeroelasiticity approach to determine the influence of model deformation [25][26][27]. Although the computational aeroelasticity method has been widely used in aircraft design [28,29], there are still some problems predicting the model deformation and variation of aerodynamic force coefficients accurately [19,30]. The third method is a combination of CFD and model deformation measurement (MDM) [31].…”
Section: Introductionmentioning
confidence: 99%
“…The approach provides a minimal order realization with exact interpolation of the unsteady aerodynamic forces in tangential directions and overcomes certain drawbacks of the classical rational function approximation approach. Boutet et al [2] discussed the development of an unsteady aerodynamic model based on the combination of Wagner theory and lifting line theory through the unsteady Kutta-Joukowski theorem. The resulting set of closed-form linear ordinary differential equations are solved analytically or by using a Runge-Kutta-Fehlberg algorithm.…”
mentioning
confidence: 99%