Characterization of a 3DOF aeroelastic system with freeplay and aerodynamic nonlinearities – Part II: Hilbert–Huang transform. (1st January 2019)

• Record Type: Journal Article
• Authors: Candon, Michael; Carrese, Robert; Ogawa, Hideaki; Marzocca, Pier; Mouser, Carl; Levinski, Oleg
• Is Part Of: Mechanical systems and signal processing. Volume 114(2019)
• Page Start: 628
• Page End: 643
• Publication Date: 2019-01-01
• Subjects: Nonlinear aeroelasticity -- System identification -- Hilbert–Huang Transform -- Structural freeplay -- Transonic flow -- Nonstationary response -- Time–frequency analysis; Structural dynamics -- Periodicals; Vibration -- Periodicals; Constructions -- Dynamique -- Périodiques; Vibration -- Périodiques; Structural dynamics; Vibration; Periodicals; 621
• DOI: 10.1016/j.ymssp.2018.04.039
• Languages: English
• ISSNs: 0888-3270

Abstract

Highlights: HHT analysis to characterize the nonlinear behavior of a 3DOF aeroelastic system with freeplay. Nonlinear modes appear, defined by complex interactions between linear aeroelastic modes. Pre-flutter the system transitions between aperiodic/chaotic and periodic response types. The transition from chaotic to periodic response is attributed to internal resonance. The ongoing periodic region is the result of a lock-in between linear and nonlinear modes. Abstract: The Hilbert–Huang Transform is used to analyze the nonlinear aeroelastic response of a 2D 3DOF aeroelastic airfoil system with control surface freeplay under transonic flow conditions. Both static and dynamic aerodynamic conditions, i . e ., for accelerating freestream speed, are considered using a linearized aerodynamic model. The main aim of this paper is to provide an in-depth physical understanding of the observed transition between periodic and aperiodic behavior, and the presence of a stable periodic region well below the domain characterized by stable limit cycles. Physical insights towards the forward and backward abrupt transition between aperiodic/chaotic and periodic behavior types appear to be the result of an internal resonance (IR) phenomenon between linear modes followed by a lock-in between linear and nonlinear modes. More specifically, initially a 2:1 IR between linear modes leads to a shift in the frequency composition and dynamic behavior of the system. A secondary effect of the IR can be observed immediately after the exact point of 2:1 IR such that a nonlinear mode locks into a subharmonic of the linear mode which in-turn drives a finite stable periodic region.