Targeted energy transfers in vibro-impact oscillators for seismic mitigation

In the field of seismic protection of structures, it is crucial to be able to diminish ‘as much as possible’ and dissipate ‘as fast as possible’ the load induced by seismic (vibration-shock) energy imparted to a structure by an earthquake. In this context, the concept of passive nonlinear energy pumping appears to be natural for application to seismic mitigation. Hence, the overall problem discussed in this paper can be formulated as follows: Design a set of nonlinear energy sinks (NESs) that are locally attached to a main structure, with the purpose of passively absorbing a significant part of the applied seismic energy, locally confining it and then dissipating it in the smallest possible time. Alternatively, the overall goal will be to demonstrate that it is feasible to passively divert the applied seismic energy from the main structure (to be protected) to a set of preferential nonlinear substructures (the set of NESs), where this energy is locally dissipated at a time scale fast enough to be of practical use for seismic mitigation. It is the aim of this work to show that the concept of nonlinear energy pumping is feasible for seismic mitigation. We consider a two degree-of-freedom (DOF) primary linear system (the structure to be protected) and study seismic-induced vibration control through the use of Vibro-Impact NESs (VI NESs). Also, we account for the possibility of attaching to the primary structure additional alternative NES configurations possessing essential but smooth nonlinearities (e.g., with no discontinuities). We study the performance of the NESs through a set of evaluation criteria. The damped nonlinear transitions that occur during the operation of the VI NESs are then studied by superimposing wavelet spectra of the nonlinear responses to appropriately defined frequency – energy plots (FEPs) of branches of periodic orbits of underlying Conservative systems.

[1]  Harry Dankowicz,et al.  Continuous and discontinuous grazing bifurcations in impacting oscillators , 2006 .

[2]  Anatoly Neishtadt Scattering By Resonances , 1997 .

[3]  Barbara Blazejczyk-Okolewska Analysis of an impact damper of vibrations , 2001 .

[4]  R. Rand The Dynamics of Resonance Capture , 2000 .

[5]  B. Brogliato Nonsmooth Mechanics: Models, Dynamics and Control , 1999 .

[6]  V. A. Pliss,et al.  Chaotic modes of oscillation of a vibro-impact system† , 2005 .

[7]  H. Nijmeijer,et al.  Dynamics and Bifurcations ofNon - Smooth Mechanical Systems , 2006 .

[8]  Alexander F. Vakakis,et al.  Energy Transfers in a System of Two Coupled Oscillators with Essential Nonlinearity: 1:1 Resonance Manifold and Transient Bridging Orbits , 2005 .

[9]  Friedrich Pfeiffer,et al.  Contacts in multibody systems , 2000 .

[10]  V. Babitsky Theory of Vibro-Impact Systems and Applications , 2013 .

[11]  Alexander F. Vakakis,et al.  Normal modes and localization in nonlinear systems , 1996 .

[12]  Oleg Gendelman,et al.  Energy pumping in nonlinear mechanical oscillators : Part I : Dynamics of the underlying Hamiltonian systems , 2001 .

[13]  Alexander F. Vakakis,et al.  Inducing Passive Nonlinear Energy Sinks in Vibrating Systems , 2001 .

[14]  Jian-Qiao Sun,et al.  Bifurcation and chaos in complex systems , 2006 .

[15]  Alexander F. Vakakis,et al.  Shock Isolation Through the Use of Nonlinear Energy Sinks , 2003 .

[16]  Steven W. Shaw,et al.  The transition to chaos in a simple mechanical system , 1989 .

[17]  Shirley J. Dyke,et al.  Next Generation Bench-mark Control Problems for Seismically Excited Buildings , 1999 .

[18]  Oleg Gendelman,et al.  ApJ, in press , 1999 .

[19]  F. Peterka,et al.  Some Aspects of the Dynamical Behavior of the Impact Damper , 2005 .

[20]  R. Storn,et al.  Differential Evolution - A simple and efficient adaptive scheme for global optimization over continuous spaces , 2004 .

[21]  Akio Tsuneda,et al.  A Gallery of attractors from Smooth Chua's equation , 2005, Int. J. Bifurc. Chaos.

[22]  Alexander F. Vakakis,et al.  Shock Isolation through Passive Energy Pumping Caused by nonsmooth nonlinearities , 2005, Int. J. Bifurc. Chaos.

[23]  Alexander F. Vakakis,et al.  Numerical and Experimental Study of Nonlinear Localization in a Flexible Structure with Vibro‐Impacts , 1997 .

[24]  Sami F. Masri,et al.  On the stability of the impact damper. , 1966 .

[25]  Sami F. Masri,et al.  Response of the impact damper to stationary random excitation , 1973 .

[26]  Aleksej F. Filippov,et al.  Differential Equations with Discontinuous Righthand Sides , 1988, Mathematics and Its Applications.

[27]  Wolfgang K. Schief,et al.  An infinite hierarchy of symmetries associated with hyperbolic surfaces , 1995 .

[28]  Rainer Storn,et al.  Differential Evolution – A Simple and Efficient Heuristic for global Optimization over Continuous Spaces , 1997, J. Glob. Optim..

[29]  V. I. Babit︠s︡kiĭ Theory of vibro-impact systems and applications , 1998 .

[30]  Gaëtan Kerschen,et al.  On the Model Validation in Nonlinear structural Dynamics , 2002 .

[31]  Alexander F. Vakakis,et al.  Irreversible Passive Energy Transfer in Coupled Oscillators with Essential Nonlinearity , 2005, SIAM J. Appl. Math..

[32]  Oleg Gendelman,et al.  Energy Pumping in Nonlinear Mechanical Oscillators: Part II—Resonance Capture , 2001 .