1988
DOI: 10.4050/jahs.33.20
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Ground and Air Resonance of an Advanced Bearingless Rotor in Hover

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Cited by 15 publications
(4 citation statements)
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“…It is important to highlight that in the literature there are different models to study the GR, such as including the stiffness of the blades, additional DOFs of fuselage and dynamics of shock absorbers mounted on the landing gears (Lytwyn et al., 1971; Janowski and Tongue, 1988; Jang and Chopra, 1998; Bielawa, 2006; Lee and Kim, 2010). However, the model used herein is also widely used for studying the GR (e.g., Coleman and Feingold, 1956; Gandhi and Malovrh, 1999; Bielawa 2006; Sanches et al., 2014; Bergeot et al., 2017), and it is employed in this work to introduce the idea of stabilizing a range of rotor speed using a single controller.…”
Section: Gr Dynamic Modelmentioning
confidence: 99%
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“…It is important to highlight that in the literature there are different models to study the GR, such as including the stiffness of the blades, additional DOFs of fuselage and dynamics of shock absorbers mounted on the landing gears (Lytwyn et al., 1971; Janowski and Tongue, 1988; Jang and Chopra, 1998; Bielawa, 2006; Lee and Kim, 2010). However, the model used herein is also widely used for studying the GR (e.g., Coleman and Feingold, 1956; Gandhi and Malovrh, 1999; Bielawa 2006; Sanches et al., 2014; Bergeot et al., 2017), and it is employed in this work to introduce the idea of stabilizing a range of rotor speed using a single controller.…”
Section: Gr Dynamic Modelmentioning
confidence: 99%
“…This phenomenon typically occurs in hinged (articulated) rotors. However, helicopters using the soft-inplane hingeless (Lytwyn et al., 1971) and bearingless rotors (Jang and Chopra, 1998) are also susceptible to this problem. A classical analysis of this phenomenon was developed by Coleman and Feingold (1956) using a simple linear mechanical model.…”
Section: Introductionmentioning
confidence: 99%
“…For the beams with no elastic couplings, the cross-sectional stiffness matrix K is given by (1) where EA is the extensional stiffness, GJ is the torsional stiffness, EI y and EI z are the flap and lag bending stiffnesses, respectively, and EC ω is the warping stiffness. For the complete details of the sectional analysis, the reader is referred to [10].…”
Section: Cross-sectional Analysismentioning
confidence: 99%
“…The coupled interaction among various disciplines, such as aerodynamics, dynamics, aeroelasticity and structures, poses a great challenge for the design of rotor blades. The bearingless main rotor (BMR) hub system lacks the conventional mechanical hinges and the pitch bearing which are used to control the blade dynamic behavior, resulting in advantages such as lower part count, lower weight, and less maintenance cost [1,2]. The BMR hub system (Fig.…”
Section: Introductionmentioning
confidence: 99%