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Journal articles on the topic 'Nonlinear vibration Absorber'

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1

Xu, Qi, Junkai Niu, Hongliang Yao, Lichao Zhao, and Bangchun Wen. "Fluid-Induced Vibration Elimination of a Rotor/Seal System with the Dynamic Vibration Absorber." Shock and Vibration 2018 (December 2, 2018): 1–15. http://dx.doi.org/10.1155/2018/1738941.

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The dynamic vibration absorbers have been applied to attenuate the rotor unbalance and torsional vibrations. The major purpose of this paper is to research the elimination of the fluid-induced vibration in the rotor/seal system using the absorber. The simplified rotor model with the absorber is established, and the Muszynska fluid force model is employed for the nonlinear seal force. The numerical method is used for the solutions of the nonlinear differential equations. The nonlinear responses of the rotor/seal system without and with the absorber are obtained, and then the rotating speed rang
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2

Habib, Giuseppe, Fanni Kádár, and Bálint Papp. "Impulsive vibration mitigation through a nonlinear tuned vibration absorber." Nonlinear Dynamics 98, no. 3 (2019): 2115–30. http://dx.doi.org/10.1007/s11071-019-05312-y.

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Abstract The dynamics of a nonlinear passive vibration absorber conceived to mitigate vibrations of a nonlinear host structure is considered in this paper. The system under study is composed of a primary system, consisting of an undamped nonlinear oscillator of Duffing type, and a nonlinear dynamic vibration absorber, denominated nonlinear tuned vibration absorber (NLTVA). The NLTVA consists of a small mass, attached to the host structure through a linear damper, a linear and a cubic spring. The host structure is subject to free vibrations and the performance of the NLTVA is evaluated with res
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3

Geeroms, M., M. Marijns, M. Loccufier, and D. Aeyels. "Design of a non-linear vibration absorber." International Journal Sustainable Construction & Design 3, no. 2 (2012): 111–15. http://dx.doi.org/10.21825/scad.v3i2.20563.

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Linear vibration absorbers can only capture certain discrete frequencies. Therefore the useof nonlinear vibration absorbers which can capture a whole range of frequencies is investigated asan alternative. Such a nonlinear vibration absorber has some special characteristics. For examplethere is a certain frequency-energy dependence. To investigate nonlinear dynamical systems thereis a need for new methods. The harmonic balance method is such a method and is discussed. Theidea is to substitute a Fourier series expansion of the solution variables into the system equations and’balance’ them. Furth
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4

Borges, R. A., A. M. G. de Lima, and V. Steffen Jr. "Robust Optimal Design of a Nonlinear Dynamic Vibration Absorber Combining Sensitivity Analysis." Shock and Vibration 17, no. 4-5 (2010): 507–20. http://dx.doi.org/10.1155/2010/587502.

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Dynamic vibration absorbers are discrete devices developed in the beginning of the last century used to attenuate the vibrations of different engineering structures. They have been used in several engineering applications, such as ships, power lines, aeronautic structures, civil engineering constructions subjected to seismic induced excitations, compressor systems, etc. However, in the context of nonlinear dynamics, few works have been proposed regarding the robust optimal design of nonlinear dynamic vibration absorbers. In this paper, a robust optimization strategy combined with sensitivity a
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5

WANG, YI-REN, and HAN-SHIANG LIN. "STABILITY ANALYSIS AND VIBRATION REDUCTION FOR A TWO-DIMENSIONAL NONLINEAR SYSTEM." International Journal of Structural Stability and Dynamics 13, no. 05 (2013): 1350031. http://dx.doi.org/10.1142/s0219455413500314.

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This study examines how the vibration absorbers influence the stability of nonlinear flow-solid interaction systems. A novel approach is proposed for the analysis of dynamic stability of the two-dimensional nonlinear system using the internal resonance contour plot (IRCP) and flutter speed contour plot (FSCP). The system considered is a planar rigid-body with plunge and pitch vibrations. The two ends of the body are supported by cubic nonlinear springs with quadratic damping. The vibration absorber attached beneath is also considered as a rigid body, with the mass and position of the absorber
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6

Sun, Xiuting, and Youshuo Song. "Dynamical Performances of a Vibration Absorber for Continuous Structure considering Time-Delay Coupling." Shock and Vibration 2016 (2016): 1–15. http://dx.doi.org/10.1155/2016/5039796.

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The nonlinear effect incurred by time delay in vibration control is investigated in this study via a vibration absorber coupled with a continuous beam structure. The stability of the vibration absorber coupled structure system with time-delay coupling is firstly studied, which provides a general guideline for the potential time delay to be introduced to the system. Then it is shown that there is a specific region for the time delay which can bring bifurcation modes to the dynamic response of the coupling system, and the vibration energy at low frequencies can be transferred or absorbed due to
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7

Xu, Qi, Junkai Niu, Hongliang Yao, Lichao Zhao, and Bangchun Wen. "Nonlinear dynamic behavior and stability of a rotor/seal system with the dynamic vibration absorber." Advances in Mechanical Engineering 11, no. 1 (2019): 168781401881957. http://dx.doi.org/10.1177/1687814018819578.

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The dynamic vibration absorbers have been applied to attenuate the critical or unbalanced vibration but may create the fluid-induced vibration instability in the rotor/seal system. The major purpose of this study is devoted to the effects of the dynamic vibration absorber on the nonlinear dynamic behavior and stability of the fluid-induced vibration in the rotor/seal system. The dynamic vibration absorber is attached on the shaft in the perpendicular directions. The model of the rotor/seal-dynamic vibration absorber system is established as the modified Jeffcott rotor system, and Muszynska non
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8

Pratt, Jon R., Shafic S. Oueini, and Alu H. Nayfeh. "Terfenol-D Nonlinear Vibration Absorber." Journal of Intelligent Material Systems and Structures 10, no. 1 (1999): 29–35. http://dx.doi.org/10.1177/1045389x9901000104.

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9

Frank Pai, P., and Mark J. Schulz. "A refined nonlinear vibration absorber." International Journal of Mechanical Sciences 42, no. 3 (2000): 537–60. http://dx.doi.org/10.1016/s0020-7403(98)00135-0.

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10

Viguié, R., and G. Kerschen. "The Nonlinear Tuned Vibration Absorber." MATEC Web of Conferences 1 (2012): 05007. http://dx.doi.org/10.1051/matecconf/20120105007.

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11

Mikhlin, Yuri V., and S. N. Reshetnikova. "Dynamical interaction of an elastic system and a vibro-impact absorber." Mathematical Problems in Engineering 2006 (2006): 1–15. http://dx.doi.org/10.1155/mpe/2006/37980.

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The nonlinear two-degree-of-freedom system under consideration consists of the linear oscillator with a relatively big mass, which is an approximation of some continuous elastic system, and of the vibro-impact oscillator with a relatively small mass, which is an absorber of the linear system vibrations. Analysis of nonlinear normal vibration modes shows that a stable localized vibration mode, which provides the vibration regime appropriate for the elastic vibration absorption, exists in a large region of the system parameters. In this regime, amplitudes of vibrations of the linear system are s
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12

Lee, Y. Y. "Analytic Formulation for the Sound Absorption of a Panel Absorber under the Effects of Microperforation, Air Pumping, Linear Vibration and Nonlinear Vibration." Abstract and Applied Analysis 2014 (2014): 1–12. http://dx.doi.org/10.1155/2014/906506.

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This study includes the first work about the absorption of a panel absorber under the effects of microperforation, air pumping, and linear and nonlinear vibrations. In practice, thin perforated panel absorber is backed by a flexible wall to enhance the acoustic performance within the room. The panel is easily excited to vibrate nonlinearly and the wall can vibrate linearly. However, the assumptions of linear panel vibration and no wall vibration are adopted in many research works. The development of the absorption formula is based on the classical approach and the electroacoustic analogy, in w
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13

Avramov, K. V., and Yu V. Mikhlin. "Snap-Through Truss as a Vibration Absorber." Journal of Vibration and Control 10, no. 2 (2004): 291–308. http://dx.doi.org/10.1177/1077546304035604.

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In this paper we consider the possibility of elastic oscillation absorption using the snap-through truss. This truss was introduced by Mises in 1923. A single-degree-of-freedom linear oscillator is chosen as the most simple model of a continuous elastic system. The nonlinear absorber with three equilibrium positions (the snap-through truss) is attached to this oscillator. The dynamics of this system is studied by the nonlinear normal vibration mode approach. The construction and stability analysis of the localized and non-localized nonlinear normal modes are developed. If the localized mode is
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14

Li, Zhi Xing, Li Hua Yang, and Qing Chao Yang. "Active Control of Nonlinear Vibration Absorber Based on Synovial Algorithm." Applied Mechanics and Materials 278-280 (January 2013): 72–78. http://dx.doi.org/10.4028/www.scientific.net/amm.278-280.72.

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In this paper, the dynamic characteristics of Duffing strong nonlinear vibration absorber system with additional hard spring is analysed qualitatively. Based on synovial variable structure algorithm, the active control system model of the nonlinear dynamic vibration absorber is designed, and the effectiveness of the control model is verified by elevant examples. It’s found that with the additional hard spring Duffing strong nonlinear vibration absorber, the control effect of active absorption is superior to the passive absorber, so which has has important guiding significance to the design of
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15

Soltani, P., and G. Kerschen. "The nonlinear piezoelectric tuned vibration absorber." Smart Materials and Structures 24, no. 7 (2015): 075015. http://dx.doi.org/10.1088/0964-1726/24/7/075015.

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16

Chen, Zhuo, and Huancai Lu. "Optimal Semiactive Damping Control for a Nonlinear Energy Sink Used to Stabilize Milling." Shock and Vibration 2020 (October 29, 2020): 1–11. http://dx.doi.org/10.1155/2020/8837753.

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Improving product quality of machining components has always met with problems due to the vibration of the milling machine’s spindle, which can be reduced by adding a vibration absorber. The tuned vibration absorber (TVA) has been studied extensively and found to have a narrow bandwidth, but the cutting force possesses wide bandwidth in the process of machining parts. Introducing nonlinearity into the dynamic vibration absorber can effectively increase the bandwidth of vibration suppression and can significantly improve the robustness of the vibration absorber. In addition, a semiactive TVA ha
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17

Habib, G., and G. Kerschen. "Suppression of limit cycle oscillations using the nonlinear tuned vibration absorber." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 471, no. 2176 (2015): 20140976. http://dx.doi.org/10.1098/rspa.2014.0976.

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The objective of this study is to mitigate, or even completely eliminate, the limit cycle oscillations in mechanical systems using a passive nonlinear absorber, termed the nonlinear tuned vibration absorber (NLTVA). An unconventional aspect of the NLTVA is that the mathematical form of its restoring force is not imposed a priori, as it is the case for most existing nonlinear absorbers. The NLTVA parameters are determined analytically using stability and bifurcation analyses, and the resulting design is validated using numerical continuation. The proposed developments are illustrated using a Va
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18

Zhang, Yu, Riccardo De Rosa, Jingyi Zhang, Mariam Alameri, and Kefu Liu. "ENERGY HARVESTING USING A NONLINEAR VIBRATION ABSORBER." Transactions of the Canadian Society for Mechanical Engineering 40, no. 2 (2016): 221–30. http://dx.doi.org/10.1139/tcsme-2016-0017.

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In this study, an energy harvesting device based on a nonlinear vibration absorber is developed to achieve two objectives: vibration suppression and energy harvesting in a wideband manner. First, the proposed design is described. Next, the system modeling is addressed. The parameter characterization is presented. Then, the performance of the nonlinear vibration absorber is tested by sweeping harmonic excitation. The testing results have shown that the device can suppress vibration and convert vibration energy into electric energy in a broadband manner.
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19

Li, Shao-Hua, Nan Liu, and Hu Ding. "Research on a nonlinear quasi-zero stiffness vibration isolator with a vibration absorber." Science Progress 103, no. 3 (2020): 003685042094089. http://dx.doi.org/10.1177/0036850420940891.

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A negative stiffness mechanism consisting of a spring and cylinder is proposed, and a grounded dynamic vibration absorber is designed based on a quasi-zero stiffness vibration isolator to constitute the vibration isolator with a vibration absorber system. The range of parameters for attaining zero stiffness is derived from static analysis. The dynamic analysis of the vibration isolator with a vibration absorber system is carried out by a multiscale method, and the amplitude–frequency response equation of the system is obtained. The influence of different system parameters on the amplitude–freq
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20

Bian, Yushu, Xuefeng Liang, and Zhihui Gao. "Vibration Reduction for a Flexible Arm Using Magnetorheological Elastomer Vibration Absorber." Shock and Vibration 2018 (2018): 1–13. http://dx.doi.org/10.1155/2018/9723538.

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The application of the magnetorheological elastomer (MRE) to nonlinear vibration control for a flexible arm is investigated in this paper. A semiactive control method is suggested to reduce vibration via the internal resonance and the MRE. To establish a vibration energy transfer channel, a tuned vibration absorber based on the MRE is developed. Through adjusting the coil current, the frequency of the vibration absorber can be readily controlled by the external magnetic field, thereby maintaining the internal resonance condition with the flexible arm. By the perturbation analysis, it is proven
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21

Lossouarn, B., J. F. Deü, and G. Kerschen. "A fully passive nonlinear piezoelectric vibration absorber." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 376, no. 2127 (2018): 20170142. http://dx.doi.org/10.1098/rsta.2017.0142.

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The objective of this study is to develop the first fully passive nonlinear piezoelectric tuned vibration absorber (NPTVA). The NPTVA is designed to mitigate a specific resonance of a nonlinear host structure. To avoid the use of synthetic inductors which require external power, closed magnetic circuits in ferrite material realize the large inductance values required by vibration mitigation at low frequencies. The saturation of an additional passive inductor is then exploited to build the nonlinearity in the NPTVA. The performance of the proposed device is demonstrated both numerically and exp
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22

Bian, Yushu, and Zhihui Gao. "Nonlinear vibration control for flexible manipulator using 1: 1 internal resonance absorber." Journal of Low Frequency Noise, Vibration and Active Control 37, no. 4 (2018): 1053–66. http://dx.doi.org/10.1177/1461348418765951.

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The main task of this paper is to put forward a vibration absorption method for attenuating nonlinear vibration of the flexible manipulator based on modal interaction. A vibration absorber is suggested to establish the 1:1 internal resonance state with the flexible manipulator, thereby transferring the vibration energy from the flexible manipulator to the vibration absorber. In the presence of damping, the vibration energy of the flexible manipulator can be effectively dissipated by the vibration absorber. Since this method puts an emphasis on constructing an internal energy transfer channel b
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23

Yan, Tinghao, Chuanbo Ren, Jilei Zhou, and Sujuan Shao. "The Study on Vibration Reduction of Nonlinear Time-Delay Dynamic Absorber under External Excitation." Mathematical Problems in Engineering 2020 (March 13, 2020): 1–11. http://dx.doi.org/10.1155/2020/8578596.

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The nonlinear time-delay dynamic absorber has a good control effect on the main system under harmonic excitation, but the control effect on the main system under complicated excitation is not obvious. In the previous study, they do not have an effective method to obtain the time-delay control parameters under different external excitations. Because of the above problems, this paper proposed an innovative method to obtain the control parameters of time-delay dynamic absorbers. For the vibration system including the nonlinear time-delay dynamic absorber, the transient time-integration method was
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24

Iurasov, Volodymyr, and Pierre-Olivier Mattei. "Vibration control with a bistale nonlinear absorber." Journal of the Acoustical Society of America 141, no. 5 (2017): 3833. http://dx.doi.org/10.1121/1.4988517.

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25

El-Bassiouny, A. F. "Internal Resonance of a Nonlinear Vibration Absorber." Physica Scripta 72, no. 2-3 (2005): 203–11. http://dx.doi.org/10.1238/physica.regular.072a00203.

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26

Raze, G., A. Jadoul, S. Guichaux, V. Broun, and G. Kerschen. "A digital nonlinear piezoelectric tuned vibration absorber." Smart Materials and Structures 29, no. 1 (2019): 015007. http://dx.doi.org/10.1088/1361-665x/ab5176.

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27

Alsuwaiyan, A. S., and Steven W. Shaw. "Steady-State Responses in Systems of Nearly-Identical Torsional Vibration Absorbers." Journal of Vibration and Acoustics 125, no. 1 (2003): 80–87. http://dx.doi.org/10.1115/1.1522420.

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In this paper we consider the steady-state response of a rotor fitted with a system of nearly identical torsional vibration absorbers. The absorbers are of the centrifugal pendulum type, which provide an effective mean of attenuating torsional vibrations of the rotor at a given order. The model considered employs absorbers that are tuned close to the order of the excitation, with an intentional mistuning that is selected by design, and imperfections among the absorbers which arise from manufacturing, wear, and other effects. It is shown that these systems can experience localized responses in
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28

Lee, Cheng-Tang, S. W. Shaw, and V. T. Coppola. "A Subharmonic Vibration Absorber for Rotating Machinery." Journal of Vibration and Acoustics 119, no. 4 (1997): 590–95. http://dx.doi.org/10.1115/1.2889766.

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We demonstrate a dynamic vibration absorber system which can be used to reduce speed fluctuations in rotating machinery. The primary system is modeled as a simple rotating disk, and the idealized absorber system consists of a pair of equal point masses which are free to move along identical, prescribed paths relative to the disk. The unique features of the proposed arrangement are that the absorbers are tuned to one-half of the frequency of the applied torque and, more importantly, that they are effective in the fully nonlinear operating range. These absorbers can, in the undamped case, exactl
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29

Konieczny, Łukasz, and Rafał Burdzik. "The use of a continuous wavelet transform in the diagnostics of technical condition of a shock absorber built in automotive vehicle." WUT Journal of Transportation Engineering 121 (June 1, 2018): 171–79. http://dx.doi.org/10.5604/01.3001.0014.4592.

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Diagnosing the technical condition of shock absorbers installed in automotive suspensions is a difficult issue due to the fact that these are elements of a complex mechanical system containing elastic and damping elements with nonlinear characteristics that degrade during operation. The paper presents the result of testing car with shock absorbers with programmed faults on the harmonic stand. The test object was a Fiat Seicento passenger car. The research experiment consisted in stimulating the vehicle to vibrations of forced masses, unsprung and sprung, and registration of vibration accelerat
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30

Tang, Bin, M. J. Brennan, G. Gatti, and N. S. Ferguson. "Experimental characterization of a nonlinear vibration absorber using free vibration." Journal of Sound and Vibration 367 (April 2016): 159–69. http://dx.doi.org/10.1016/j.jsv.2015.12.040.

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31

Tang, Si Mi, Shi Jian Zhu, and Jing Jun Lou. "Study on Dynamics of a Nonlinear Damping Absorber Coupled to the Linear System." Advanced Materials Research 143-144 (October 2010): 763–67. http://dx.doi.org/10.4028/www.scientific.net/amr.143-144.763.

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The dynamics of a two degree-of-freedom (DOF) system consisting of a linear system coupled with a quadratic damping vibration absorber is studied. The nonlinear energy pumping phenomenon is verified by simulation and analyzed by Hilbert Transform. Performance of the quadratic damping absorber that is able to absorb vibration over a broad range of frequency (nonlinear energy sink, NES) is studied, and the results are compared with that of the classical linear vibration absorber. The relationship between parameters and performance of the absorber is analyzed, that is significant for engineering
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32

Wei, Y. M., X. J. Dong, P. F. Guo, Z. K. Peng, and W. M. Zhang. "Enhanced Targeted Energy Transfer by Vibro Impact Cubic Nonlinear Energy Sink." International Journal of Applied Mechanics 10, no. 06 (2018): 1850061. http://dx.doi.org/10.1142/s1758825118500618.

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Passive targeted energy transfer (TET) that describes a highly efficient manner of energy absorption is considerably enhanced by a new form of absorber proposed in this paper. The absorber is attached to the primary linear oscillator (LO) through cubic stiffness and bilateral barriers that set to induce vibro-impact (VI). Both essential nonlinearity and non-smooth nonlinearity are considered. Energy pumping phenomenon is found, and complexification averaging method is used to give an analytical treatment for the essential stiffness nonlinearity. At a low level of impulse excitation where energ
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33

Yabuno, Hiroshi, Ryo Kanda, Walter Lacarbonara, and Nobuharu Aoshima. "Nonlinear Active Cancellation of the Parametric Resonance in a Magnetically Levitated Body." Journal of Dynamic Systems, Measurement, and Control 126, no. 3 (2004): 433–42. http://dx.doi.org/10.1115/1.1789530.

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An active control strategy for the stabilization of parametric resonance in a magnetically levitated body is proposed. The characteristic feature of the strategy is the exploitation of the nonlinear effect of the inertial force associated with the motion of a pendulum-type vibration absorber driven by an appropriate control torque. As a distinguished feature, the proposed control method does not rely on the effective autoparametric energy transfer between the main system and the absorber. Because the main system is not linearly coupled with the absorber, the drawback inherent in the increase o
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34

Dimentberg, M., S. Chen, Z. Hou, and M. Noori. "Tuned Vibration Absorbers For Floating Bodies." Journal of Vibration and Control 2, no. 4 (1996): 415–29. http://dx.doi.org/10.1177/107754639600200403.

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A preliminary feasibility study is made of the efficiency of tuned vibration absorbers for reducing response of floating bodies, such as offshore platforms, barges, and so on, to random ocean waves. The absorbers are submerged spring-loaded flaps, with stiffnesses of the springs being adjusted for tuning to any specific (rigid-body) mode of the platform (heaving, pitching, etc.), whereas actual design of the flaps should provide the desired amount of drag-induced damping. Mean square response analysis of the system is made for the case of a narrow-band random excitation due to ocean waves by u
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35

LI, S. B., W. ZHANG, and M. H. YAO. "USING ENERGY-PHASE METHOD TO STUDY GLOBAL BIFURCATIONS AND SHILNIKOV TYPE MULTIPULSE CHAOTIC DYNAMICS FOR A NONLINEAR VIBRATION ABSORBER." International Journal of Bifurcation and Chaos 22, no. 01 (2012): 1250001. http://dx.doi.org/10.1142/s0218127412500010.

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Global bifurcations and Shilnikov type multipulse chaotic dynamics for a nonlinear vibration absorber are investigated by using the energy-phase method for the first time. A two-degree-of-freedom model of a nonlinear vibration absorber is considered. After the nonlinear nonautonomous equations of this model are given, the method of multiple scales is used to derive four first-order nonlinear ordinary differential equations governing the modulation of the amplitudes and phases of the two interacting modes in the presence of 1:1 internal resonance and primary resonance. Using several coordinate
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36

Casalotti, Arnaldo, and Walter Lacarbonara. "Nonlinear Vibration Absorber Optimal Design via Asymptotic Approach." Procedia IUTAM 19 (2016): 65–74. http://dx.doi.org/10.1016/j.piutam.2016.03.010.

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37

YUKI, Takao, Kaoru UTSUNOMIYA, Yoshihiro TSUDA, and Atsuo SUEOKA. "306 The Dynamics of a Nonlinear Vibration Absorber." Proceedings of Conference of Kyushu Branch 2000 (2000): 77–78. http://dx.doi.org/10.1299/jsmekyushu.2000.77.

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38

Chung, Chiou-Fong, Pi-Cheng Tung, and Chiang-Nan Chang. "Dynamics Analysis of an Asymmetric Nonlinear Vibration Absorber." Japanese Journal of Applied Physics 41, Part 1, No. 10 (2002): 6276–82. http://dx.doi.org/10.1143/jjap.41.6276.

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39

Oueini, Shafic S., and Ali H. Nayfeh. "Analysis and Application of a Nonlinear Vibration Absorber." Journal of Vibration and Control 6, no. 7 (2000): 999–1016. http://dx.doi.org/10.1177/107754630000600703.

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40

Habib, G., G. Kerschen, and G. Stepan. "Chatter mitigation using the nonlinear tuned vibration absorber." International Journal of Non-Linear Mechanics 91 (May 2017): 103–12. http://dx.doi.org/10.1016/j.ijnonlinmec.2017.02.014.

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41

Egorov, Vladimir, and Grigory Belyy. "Nonlinear properties of hybrid construction of coatings of buildings and structures." E3S Web of Conferences 217 (2020): 01001. http://dx.doi.org/10.1051/e3sconf/202021701001.

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Stress and strain state of hybrid (combined) systems including flexible and rigid elements is studied in the article. Theoretical approach is presented. The feature of the systems studied is described, i.e. structural nonlinearity. Numerical analysis is presented. It is pointed out that vibrations of such structures upon conditions of resonance differ from those of classical bar structures, i.e. if for rigid bar systems the amplitudes of vibration at resonant disturbance increase monotonously, in combined (hybrid) system alternate switching off tie-bars stabilizes the amplitude of vibration at
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42

Gao, Zhi Hui, Bing Dong Liu, and Bo Shan. "Vibration Control of the Flexible Robotic Arm through Modal Interaction." Applied Mechanics and Materials 490-491 (January 2014): 1142–45. http://dx.doi.org/10.4028/www.scientific.net/amm.490-491.1142.

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A vibration control method is proposed to suppress nonlinear large vibration of the flexible robotic arm undergoing rigid motion. The method takes advantage of modal interaction and is implemented based on internal resonance. To attenuate vibration of the flexible arm, another vibrating system, consisting of a rigid link, a flexible joint and a damper, is introduced as a vibration absorber. Perturbation technique is used to study the transient response of the nonlinear equations of motion. Numerical simulation results preliminarily verify that the proposed control strategy is able to effective
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43

Dong, Guangxu, Qiang Li, and Xinong Zhang. "Vibration attenuation using a nonlinear dynamic vibration absorber with negative stiffness." International Journal of Applied Electromagnetics and Mechanics 59, no. 2 (2019): 617–28. http://dx.doi.org/10.3233/jae-171201.

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44

Bian, Yushu, Zhihui Gao, and Ming Fan. "Nonlinear Vibration Suppression for Flexible Arms via Modal Coupling." International Journal of Structural Stability and Dynamics 17, no. 03 (2017): 1771004. http://dx.doi.org/10.1142/s0219455417710043.

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Modal coupling is an important characteristic of most nonlinear dynamic systems. Although the existence of modal coupling can make the dynamic responses of a system quite complicated, it can be utilized to provide potential solutions to regulate nonlinear vibration. In this paper, the mechanism of modal coupling is used as a means to suppress vibration of a flexible arm undergoing joint motion. A secondary oscillatory system is attached to the flexible arm to generate appropriate modal coupling. Via this nonlinear coupling, internal resonance can be successfully induced and used to transfer vi
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Yao, Hongliang, Zidong Chen, and Bangchun Wen. "Dynamic Vibration Absorber with Negative Stiffness for Rotor System." Shock and Vibration 2016 (2016): 1–13. http://dx.doi.org/10.1155/2016/5231704.

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To suppress the vibration of a rotor system, a vibration absorber combining negative stiffness with positive stiffness together is proposed in this paper. Firstly, the negative stiffness producing mechanism using ring type permanent magnets is presented and the characteristics of the negative stiffness are analyzed. Then, the structure of the absorber is proposed; the principles and nonlinear dynamic characteristics of the absorber-rotor system are studied numerically. Finally, experiments are carried out to verify the numerical conclusions. The results show that the proposed vibration absorbe
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46

KOJIMA, Hiroyuki, and Kosuke NAGAYA. "Forced Vibrations of a Circular Plate with a Nonlinear Dynamic Vibration Absorber." Bulletin of JSME 28, no. 236 (1985): 309–14. http://dx.doi.org/10.1299/jsme1958.28.309.

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47

Piccirillo, Vinícius, José M. Balthazar, Angelo Marcelo Tusset, Davide Bernardini, and Giuseppe Rega. "Application of a Shape Memory Absorber in Vibration Suppression." Applied Mechanics and Materials 849 (August 2016): 27–35. http://dx.doi.org/10.4028/www.scientific.net/amm.849.27.

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The dynamic response of structures subjected to high-amplitude vibration is often dangerous and undesirable. Dynamic vibration absorbers (DVA) have received special attention in recent years due to vibration attenuation offered by them. Thus, the present study analyzes the nonlinear dynamics of a system with a dynamic vibration absorber (DVA) using a shape memory material (SMM) whose characteristics are highly dependent upon temperature. The restoring force of the oscillator is provided by a shape-memory device (SMD) described by a thermomechanical model capable to describe the hysteretic beha
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48

ZHANG, WEI, and JING LI. "GLOBAL ANALYSIS FOR A NONLINEAR VIBRATION ABSORBER WITH FAST AND SLOW MODES." International Journal of Bifurcation and Chaos 11, no. 08 (2001): 2179–94. http://dx.doi.org/10.1142/s0218127401003334.

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A two-degree-of-freedom model of a nonlinear vibration absorber is considered in this paper. Both the global bifurcations and chaotic dynamics of the nonlinear vibration absorber are investigated. The nonlinear equations of motion of this model are derived. The method of multiple scales is used to find the averaged equations. Based on the averaged equations, the theory of normal form is used to obtain the explicit expressions of normal form associated with a double zero and a pair of pure imaginary eigenvalues by Maple software program. The fast and slow modes may simultaneously exist in the a
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Abundis-Fong, H. F., J. Enríquez-Zárate, A. Cabrera-Amado, and G. Silva-Navarro. "Optimum Design of a Nonlinear Vibration Absorber Coupled to a Resonant Oscillator: A Case Study." Shock and Vibration 2018 (2018): 1–11. http://dx.doi.org/10.1155/2018/2107607.

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This paper presents the optimal design of a passive autoparametric cantilever beam vibration absorber for a linear mass-spring-damper system subject to harmonic external force. The design of the autoparametric vibration absorber is obtained by using an approximation of the nonlinear frequency response function, computed via the multiple scales method. Based on the solution given by the perturbation method mentioned above, a static optimization problem is formulated in order to determine the optimum parameters (mass and length) of the nonlinear absorber which minimizes the steady state amplitud
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Wang, Xi, and Bintang Yang. "Transient vibration control using nonlinear convergence active vibration absorber for impulse excitation." Mechanical Systems and Signal Processing 117 (February 2019): 425–36. http://dx.doi.org/10.1016/j.ymssp.2018.07.038.

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