Nonlinear tuned mass dampers (TMDs) are widely recognized for their superior damping perfor-mance, which stems from their broad damping bandwidth. In this study, we propose a sin-gle-pendulum TMD for application in vibration absorption within train compressors to protect crit-ical components. However, the inherent nonlinear vibration characteristics of the TMD may under-mine its damping effectiveness. To address this challenge, we develop a three-degree-of-freedom mechanical model of a train compressor integrated with a single-pendulum TMD. The equations of motion for the system are derived using the second kind of Lagrange formula. By employing the fourth-order Runge-Kutta numerical integration method and using the excitation frequency as the bifurcation parameter, we analyze the bifurcation behavior and the transition to chaos via the Poin-caré cross-section method. Our results demonstrate that the system can transition to chaos through multiple routes, including multiplicative bifurcation, Hopf bifurcation, and residual-dimension bi-furcation, depending on the excitation frequency. These findings provide critical insights for the dynamic design and chaotic motion prediction of single-pendulum TMD systems, offering practical guidance to enhance their reliability and performance in real-world applications.
Citation: Danyang Wang, Ning Chen. Research on Hopf bifurcation of vehicle air compressor system with single-pendulum TMD[J]. Electronic Research Archive, 2025, 33(5): 3285-3304. doi: 10.3934/era.2025145
Nonlinear tuned mass dampers (TMDs) are widely recognized for their superior damping perfor-mance, which stems from their broad damping bandwidth. In this study, we propose a sin-gle-pendulum TMD for application in vibration absorption within train compressors to protect crit-ical components. However, the inherent nonlinear vibration characteristics of the TMD may under-mine its damping effectiveness. To address this challenge, we develop a three-degree-of-freedom mechanical model of a train compressor integrated with a single-pendulum TMD. The equations of motion for the system are derived using the second kind of Lagrange formula. By employing the fourth-order Runge-Kutta numerical integration method and using the excitation frequency as the bifurcation parameter, we analyze the bifurcation behavior and the transition to chaos via the Poin-caré cross-section method. Our results demonstrate that the system can transition to chaos through multiple routes, including multiplicative bifurcation, Hopf bifurcation, and residual-dimension bi-furcation, depending on the excitation frequency. These findings provide critical insights for the dynamic design and chaotic motion prediction of single-pendulum TMD systems, offering practical guidance to enhance their reliability and performance in real-world applications.
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