Abstract

Seismic isolation devices are usually designed to protect structures from the strong horizontal component of earthquake ground shaking. However, the effect of near-fault (NF) vertical ground motions on seismic responses of buildings has become an important consideration due to the observed building damage caused by vertical excitation. As the structure needs to maintain its load bearing capacity, using the horizontal isolation strategy in vertical seismic isolation will lead to the problem of larger static displacement. In particular, the bearings may generate large deformation responses of isolators for NF vertical ground motions. A seismic isolation system including quasi-zero stiffness (QZS) and vertical damper (VD) is used to control NF vertical earthquakes. The characteristics of vertical seismic isolated structures incorporating QZS and VD are presented. The formula for the maximum bearing capacity of QZS isolation considering the stiffness of vertical spring components is obtained by theoretical derivation. From the static analysis, it is found that the static capacity of the QZS isolation system with vertical seismic isolation components increases when the configurative parameter reduces. Seismic response analyses of the seismic isolated structure model with QZS and VD subjected to NF vertical earthquakes are conducted. The results show that seismic responses of the structure can be controlled by setting the appropriate static equilibrium position, vertical isolation period, and vertical damping ratio. Adding a damping ratio is effective in controlling the vertical large deformation of the isolator.

Highlights

  • Seismic isolation is one of most effective control ways to protect structural systems, nonstructural systems, and content from damage due to horizontal earthquake ground motions [1, 2]

  • It has been found that the vertical-to-horizontal acceleration (V/H) response spectral ratios are strongly dependent on period and site-to-source distance during the 1994 Northridge earthquake [4]

  • When the mass oscillation reaches the steady state around the static equilibrium position, the dynamic equilibrium can be established as mÿ + 2k (1 − L ) y + kVy + cVẏ = − myg, (13) √a2 + y2 which can be written in a nondimensional form as ŷ + 2ω2β (1 − 1 ) ŷ + ω2ŷ + 2ωξŷ = − ŷg, (14) √γ2 + ŷ2 where ŷ = y/L, ŷg = yg/L, ω2 = kV/m, ξ = cV/2mωV, and T = 2π√m/kV

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Summary

Introduction

Seismic isolation is one of most effective control ways to protect structural systems, nonstructural systems, and content from damage due to horizontal earthquake ground motions [1, 2]. Focused on NF vertical seismic protection of structures such as span systems and base-isolated structures [3, 14], the objective of this study is to present a vertical isolation system that has sufficient static vertical rigidity to prevent large static deformations due to the self-weight of supported structures, while having enough dynamic flexibility and energy dissipation to reduce NF vertical seismic responses. This approach is different from the horizontal isolation strategy. Comparison analyses of the QZS system and the seismic isolated system without QZS are presented to check the isolation effectiveness for the model against NF vertical ground motions

Seismic Isolated Structure Model with QZS
Static Performance
Dynamic Equation of Motion for Seismic Input
Selection of Near-Fault Vertical Ground Motion Records
Seismic Response Analysis
Parameter Design and Performance Evaluation
Conclusions
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