2021
DOI: 10.1007/978-3-030-74236-2_11
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Nonlinear Aeroelasticity

Abstract: This is an introduction and overview of the work that has been done in nonlinear aeroelasticity prior to the last decade. Many of the issues discussed here are still under active investigation. Of particular interest are the limit cycle oscillations that may occur once the dynamic stability (flutter) boundary has been exceeded.

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Cited by 6 publications
(13 citation statements)
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“…In terminology of the work [10], the 'Ziegler's double pendulum' is a MDKN-system due to absence of gyroscopic forces, which are typical in the reduced order models of fluidstructure interaction problems of aeroelasticity [1,3,4] thus representing MDGKN systems [10].…”
Section: (A) the Counterintuitive Character Of Flutter Instabilitymentioning
confidence: 99%
See 1 more Smart Citation
“…In terminology of the work [10], the 'Ziegler's double pendulum' is a MDKN-system due to absence of gyroscopic forces, which are typical in the reduced order models of fluidstructure interaction problems of aeroelasticity [1,3,4] thus representing MDGKN systems [10].…”
Section: (A) the Counterintuitive Character Of Flutter Instabilitymentioning
confidence: 99%
“…The latter assumption holds when the structural vibrations can be neglected as characterized by a velocity much smaller than that of the fluid flow. Under this circumstance, the coupling between the structure and the fluid reduces to a weak coupling and so the aeroelastic force F a can be approximated at small amplitude vibrations as [1,4,28]…”
Section: (A) the Counterintuitive Character Of Flutter Instabilitymentioning
confidence: 99%
“…The dynamic similarity law for the FSI consists of four nondimensional parameters: 𝛼, Re, Ca, and R M are, respectively, the ratio of the inertial force due to the local acceleration to that due to the advection, 98 the Reynolds number or the ratio of the inertial force due to the advection to the viscous force, 98 the Cauchy number or the ratio of the fluid dynamic pressure to the structural elastic force, 99 and the (solid-to-fluid) mass ratio, 100,101 which are written with respect to the characteristic length L, the characteristic velocity V, and the characteristic time T as follows…”
Section: Basic Verification Of the Algorithm And The Implementation C...mentioning
confidence: 99%
“…Here, we impose the so‐called impermeability condition on Ω; namely, we assume that no fluid passes through the elastic portion of the boundary during deflection [15, 28]. Also, note that the FSI problem under consideration has a material derivative term on the deflected interaction surface, which computes the time rate of change of any quantity such as temperature or velocity (and hence also acceleration) for a portion of a material in motion.…”
Section: Introductionmentioning
confidence: 99%