2017
DOI: 10.1007/s00348-017-2382-2
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Drag reduction of a car model by linear genetic programming control

Abstract: We investigate open-and closed-loop active control for aerodynamic drag reduction of a car model. Turbulent flow around a blunt-edged Ahmed body is examined at Re H ≈ 3 × 10 5 based on body height. The actuation is performed with pulsed jets at all trailing edges combined with a Coanda deflection surface. The flow is monitored with pressure sensors distributed at the rear side. We apply a model-free control strategy building on Dracopoulos & Kent (1997) and Gautier et al. (2015). The optimized control laws com… Show more

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Cited by 74 publications
(71 citation statements)
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“…In the second numerical example, a flow past a cylinder was simulated. The problem domain is nondimensional 50 units in length and nondimensional 10 units in width, and it possesses a cylinder of radius nondimensional 3 units positioned over the point (5,5). Figure 6 shows the computational domain, with a mesh of 3213 nodes.…”
Section: Flow Past a Cylindermentioning
confidence: 99%
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“…In the second numerical example, a flow past a cylinder was simulated. The problem domain is nondimensional 50 units in length and nondimensional 10 units in width, and it possesses a cylinder of radius nondimensional 3 units positioned over the point (5,5). Figure 6 shows the computational domain, with a mesh of 3213 nodes.…”
Section: Flow Past a Cylindermentioning
confidence: 99%
“…Thus, even with moderate complexity problems, the computation cost can still be prohibitive. A number of model identification methods have been presented to improve the capabilities of the mathematical models such as state calibration with 4D Var, 1 neural networks, 2 dynamics with radial basis functions, 3 genetic programming, 2,4,5 and the traditional Galerkin method. 1,6 Reduced order modelling, one of model identification methods, has proven to be a powerful tool to reduce the complexity and large dimensional size of the full discretised dynamical system.…”
mentioning
confidence: 99%
“…Thus, the number of possible duty cycles N DC for a given f is N DC = N sp − 1 = F RT / f − 1, which increases with N sp and decreases with f . This process is similar to that used in Li et al (2017). Figure 2 displays the permitted frequencies and duty cycles and shows the manually selected frequencies which allow for a locally maximum number of duty cycles.…”
Section: Real-time Systemmentioning
confidence: 99%
“…The larger k ∈ (−1, 1), the smaller the duty cycle. Following Li et al (2017), a much more general multifrequency forcing is considered, generated here by 9 harmonic functions h i = sin(2π f i t), i = 1, . .…”
Section: Multi-frequency Forcingmentioning
confidence: 99%
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