带有摩擦张力装置的摇摆框架的性能

IF 0.8 Q4 ENGINEERING, GEOLOGICAL Bulletin of the New Zealand Society for Earthquake Engineering Pub Date : 2023-06-01 DOI:10.5459/bnzsee.1583
Kiran Rangwani, G. MacRae, G. Rodgers
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引用次数: 0

摘要

介绍了一种新的仅摩擦张力的“GripNGrab”装置在摇摆钢架上的实现。当受到显著张力时,该装置通过在摩擦部件中滑动来耗散能量。当装置在压缩方向上加载时,几乎不携带压缩力,但棘轮部件中发生位移。耗散系统中没有任何显著的压缩力,这意味着摇摆框架在地震震动引起的隆起后总是会重新集中。设计了一个高9米、宽4.75米的3层钢制同心支撑摇摆框架,具有低损伤抗震性能。恢复力由(i)重力、(ii)底部的摩擦“GripNGrab”(GNG)纯张力耗散装置和(iii)梁板效应提供。该结构的初始基本周期为0.16s。初始结构使用10mm的GNG棘轮节距,并且具有在正常使用水平振动下不滑动的GNG强度。使用OpenSEES软件对不同振动强度的弹性、推覆、循环推覆以及时间历程进行了分析。工程范围仅限于单个建筑和单个地面运动。变化的参数包括梁板效应的存在,以及GNG装置的刚度、强度和齿距。结果表明,考虑到循环pushover分析,可以理解框架的全部行为。峰值隆起位移是使用刚体力学根据峰值屋顶位移保守估计的,并且仅限张力的装置对全框架重新定心没有阻力。对于所考虑的框架,确定仅受拉装置的非弹性位移能力所必需的累积上拔位移高达峰值上拔位移的28倍,而不一定发生在最大震动强度下。最大框架基础剪力需求是推倒分析的1.43倍。当梁板将摇摆框架连接到结构的其余部分时,增加了侧向力阻力,基底剪力显著增加,减少了屋顶的峰值位移,并增加了峰值隆起位移循环的有效次数(NPUDc)。对于大的振动强度,梁板发生屈服,导致永久性的峰值屋顶和隆起位移。在所研究的情况下,GNG装置的强度、刚度和齿距变化对响应没有显著影响。对于这些具有较小能量耗散的短周期结构,基于初始刚度和割线刚度的方法预测摇摆框架的响应是非保守的,并且针对所研究的基于一系列振动强度的R-T-m关系的情况,开发了一种简单的改进来匹配行为。
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Performance of rocking frames with friction tension-only devices
The implementation of a new friction tension-only “GripNGrab” device attached to a rocking steel frame is described. The device, when subject to significant tension dissipates energy via sliding in the frictional component. When the device is loaded in the compression direction, almost no compressive force is carried, but displacement occurs in the ratchetting component. This absence of any significant compressive force within the dissipative system means that the rocking frame will always recentre after uplift from earthquake shaking. A 9 m tall 4.75m wide 3-storey steel concentrically braced rocking frame is designed for low-damage seismic performance. Restoring forces are provided by (i) gravity, (ii) friction “GripNGrab” (GNG) tension-only dissipation devices at the base, and (iii) beam-slab effects. The initial fundamental period of the structure was 0.16s. The initial structure used a 10mm GNG ratchet pitch, and had a GNG strength to not slide under serviceability level shaking. Elastic, pushover, cyclic pushover, as well as time history analyses, with different shaking intensities are conducted using OpenSEES software. The scope of work is limited to a single building and a single ground motion. Parameters varied included the presence of beam-slab effects, and the GNG device stiffness, strength and tooth pitch. It is shown that the full behaviour of the frame could be understood considering cyclic pushover analysis. The peak uplift displacement was conservatively estimated from the peak roof displacement using rigid body mechanics and the tension-only device provided no resistance to full frame recentring. For the frames considered, cumulative uplift displacements, necessary to determine the inelastic displacement capacity of the tension only device, were up to 28 times the peak uplift displacement, not necessarily occurring at the maximum shaking intensity. Maximum frame base shear force demands were up to 1.43 times that from pushover analysis. When the beam-slab, connecting the rocking frame to the rest of the structure, increased the lateral force resistance, the base shear increased significantly, reduced peak roof displacements, and increased the effective number of peak uplift displacement cycles (NPUDc). For large shaking intensities, yielding of the beam-slab occurred resulting in permanent peak roof and uplift displacements. The GNG device strength, stiffness and tooth pitch variations for the cases studied did not significantly affect the response. Initial stiffness, and secant stiffness, based methods to predict the response of rocking frames were non-conservative for these short-period structures with small energy dissipation, and a simple improvement to match the behaviour was developed for the case studied based on the R-T-m relationship for a range of shaking intensity.
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2.50
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17.60%
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14
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