2001
DOI: 10.1106/hmnl-vdkd-u3tr-4xwa
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Performance Comparison between Piezoelectric and Elastomeric Lag Dampers on Ground Resonance Stability of Helicopter

Abstract: In this study, a piezoelectric lag damper using damping characteristics in piezoelectric ceramics is proposed to alleviate ground resonance instability. The piezoelectric passive damper consists of piezoelectric elements and electrical circuits such as resistors and inductors in a series. By bonding the piezoelectric ceramics to the rotor flexures, piezoelectric strain energy is converted to electrical energy and dissipated through an electrical network. To verify the effect of the piezoelectric damper on rota… Show more

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Cited by 8 publications
(4 citation statements)
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“…According to the literature, for this problem aerodynamic effects can be neglected (Coleman and Feingold, 1956; Hammond,. 1974; Janowski and Tongue, 1988; Gandhi and Malovrh, 1999; Kim and Yun, 2001; Kunz, 2002; Zhao et al., 2004; Bielawa, 2006; Bauchau et al., 2010; Sanches et al., 2011, 2012, 2014; Bergeot et al., 2016, 2017); however, this is dependent on the levels of flexibility and rotor speed. Also, the fuselage and the blade structural damping are neglected because the dissipative nature of damping contributes to stabilize the system.…”
Section: Gr Dynamic Modelmentioning
confidence: 99%
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“…According to the literature, for this problem aerodynamic effects can be neglected (Coleman and Feingold, 1956; Hammond,. 1974; Janowski and Tongue, 1988; Gandhi and Malovrh, 1999; Kim and Yun, 2001; Kunz, 2002; Zhao et al., 2004; Bielawa, 2006; Bauchau et al., 2010; Sanches et al., 2011, 2012, 2014; Bergeot et al., 2016, 2017); however, this is dependent on the levels of flexibility and rotor speed. Also, the fuselage and the blade structural damping are neglected because the dissipative nature of damping contributes to stabilize the system.…”
Section: Gr Dynamic Modelmentioning
confidence: 99%
“…Considering the first-time derivative of equation (1) and introducing the result into equation (2c), the blade's kinetic energy is accounted for. Then, substituting the energy expressions (equations (2a)–(3c)) in the Lagrange's equations (equations (38a)–(38c)) considering the absence of external forces acting on the system, the equations of motion can be derived as Following Coleman and Feingold (1956), Hammond (1974), Janowski and Tongue (1988), Gandhi and Malovrh (1999); Kim and Yun (2001), Kunz (2002), Zhao et al. (2004), Bielawa (2006), Bauchau et al.…”
Section: Appendix A: Proof Of Theoremmentioning
confidence: 99%
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