2021
DOI: 10.1016/j.compstruc.2020.106359
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First-excursion stochastic incremental dynamics methodology for hysteretic structural systems subject to seismic excitation

Abstract: A novel efficient stochastic incremental dynamics methodology considering first-excursion probability for nonlinear structural systems subject to stochastic seismic excitations in alignment with contemporary aseismic codes provisions is developed. To this aim, an approximate nonlinear stochastic dynamics technique for conducting first-passage probability density function (PDF) based stochastic incremental dynamic analysis is developed. Firstly, an efficient stochastic iterative linearization methodology is dev… Show more

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Cited by 6 publications
(5 citation statements)
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“…If Xi(t)$X_i(t)$ is the obtained stochastic response process, the pseudo‐acceleration response spectrum is: Sa(ωi,ζ)badbreak=ηXiωi2λ0,Xi$$\begin{equation} S_a^*(\omega _i,\zeta) = \eta _{X_i}\omega _i^2\sqrt {\lambda _{0,X_i}} \end{equation}$$where ηXi$\eta _{X_i}$ is the peak factor and λ0,Xi$\lambda _{0,X_i}$ is the variance of the stochastic response process Xi(t)$X_i(t)$. The peak factor ηXi$\eta _{X_i}$ is the critical factor by which the standard deviation λ0,Xi$\sqrt {\lambda _{0,X_i}}$ of the considered elastic oscillator response is multiplied to predict a level of spectral acceleration Sa(ωi,ζ)$S_a^*(\omega _i,\zeta)$ below which the peak response will remain in the interval of Ts$T_s$, with probability p$p$ 46 . The ”s$_s$” in Ts$T_s$ and Gs(ωi…”
Section: Preliminary Concepts: the Spectral Representation Methodsmentioning
confidence: 99%
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“…If Xi(t)$X_i(t)$ is the obtained stochastic response process, the pseudo‐acceleration response spectrum is: Sa(ωi,ζ)badbreak=ηXiωi2λ0,Xi$$\begin{equation} S_a^*(\omega _i,\zeta) = \eta _{X_i}\omega _i^2\sqrt {\lambda _{0,X_i}} \end{equation}$$where ηXi$\eta _{X_i}$ is the peak factor and λ0,Xi$\lambda _{0,X_i}$ is the variance of the stochastic response process Xi(t)$X_i(t)$. The peak factor ηXi$\eta _{X_i}$ is the critical factor by which the standard deviation λ0,Xi$\sqrt {\lambda _{0,X_i}}$ of the considered elastic oscillator response is multiplied to predict a level of spectral acceleration Sa(ωi,ζ)$S_a^*(\omega _i,\zeta)$ below which the peak response will remain in the interval of Ts$T_s$, with probability p$p$ 46 . The ”s$_s$” in Ts$T_s$ and Gs(ωi…”
Section: Preliminary Concepts: the Spectral Representation Methodsmentioning
confidence: 99%
“…The peak factor 𝜂 𝑋 𝑖 is the critical factor by which the standard deviation √ 𝜆 0,𝑋 𝑖 of the considered elastic oscillator response is multiplied to predict a level of spectral acceleration 𝑆 * 𝑎 (𝜔 𝑖 , 𝜁) below which the peak response will remain in the interval of 𝑇 𝑠 , with probability 𝑝. 46 The " 𝑠 " in 𝑇 𝑠 and 𝐺 𝑠 (𝜔 𝑖 ) refers to stationarity. The evaluation of 𝜂 𝑋 𝑖 is related to the concept of the first-passage problem.…”
Section: Spectral Representation Technique For the Stationary Casementioning
confidence: 99%
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“…The stochastic component x s (t) of the system response is treated by resorting to the generalized statistical linearization methodology for systems with singular parameter matrices [12,13]; see also [16,17,18,19,20,21,22,23] for a broader perspective, as well as several examples pertaining to application of the method. First, the difference between the systems in Eqs.…”
Section: Application Of the Statistical Linearization Methods For Treating The Stochastic Component Of The Responsementioning
confidence: 99%