2010
DOI: 10.1177/1475921710368202
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Instantaneous Identification of Degrading Hysteretic Oscillators Under Earthquake Excitation

Abstract: This article presents a technique for the structural identification of hysteretic oscillators that are characterized by degradation in stiffness. The main assumption of the proposed procedure is that it is possible to replace the expression of the time derivative of the restoring force with a polynomial approximation, characterized by time-varying coefficients. The work aims at generalizing a method that the authors have proposed for hysteretic nondegrading systems: system parameters are evaluated from instant… Show more

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Cited by 9 publications
(5 citation statements)
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“…Comparing (5) with (1) it is possible to find the unknown linear parameters, , supposing to know while solving the system of equations (2). can be found by using numerical algorithms that minimize the cost function, , for the d-th DoF: (12) where te is the length of the signals and T denotes the linear TFD operator.…”
Section: The 3 Dofs Black-box Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…Comparing (5) with (1) it is possible to find the unknown linear parameters, , supposing to know while solving the system of equations (2). can be found by using numerical algorithms that minimize the cost function, , for the d-th DoF: (12) where te is the length of the signals and T denotes the linear TFD operator.…”
Section: The 3 Dofs Black-box Modelmentioning
confidence: 99%
“…Another important classification of the identification methods for nonlinear systems is based on the domain in which the identification is performed: frequency, time, or joint time-frequency domain, e.g. [11], [12]. Using a joint time-frequency domain can be also useful to perform instantaneous estimates of the parameters value, whose stability over time is symptom of consistency of a given model, [13].…”
Section: Introductionmentioning
confidence: 99%
“…The parametric identification described above was applied to the three‐dimensional structure depicted in Figure (b), subject to the four levels of PGA reported in Table . The identification algorithm described at length in minimised the objective function Q ( t , p ) expressed in (5). In greater detail, Q ( t , p ) was extended to a 2‐DOF system as follows: Qj,p=i=12k=0N1SPECxi()γj,k;pSPECxim()γj,kboldpitalicidt¯=j¯Δt=argminp,j=j¯Qj,pwhere p = { k 11 , k 12 , k 22 , β 1 , β 2 , γ 1 , γ 2 , n 1 , n 2 , s 1 , s 2 , μ s 1 , μ s 2 } defines the vector of linear, hysteretic and slip parameters, respectively, referred to the system (21).…”
Section: Parametric Identification Of the Condensed 2‐dof Systemmentioning
confidence: 99%
“…In addition, the availability of hysteretic mathematical models easily allows for the development of control laws for nonlinear structural hysteretic systems . Within this framework, our research tries to combine the benefit of: (i) the classical pseudodynamic (PsD) testing technique, as applied to structures for which strain‐rate effects can be neglected , and (ii) nonlinear identification techniques of complex nonlinear systems, capable of capturing hereditary characteristics of inelastic restoring forces of structures .…”
Section: Introductionmentioning
confidence: 99%
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