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1.
李福民 《地震学报》1982,4(3):301-307
本文用数值积分法,对RDZ1-12-66型自动触发电流计记录式强震仪的幅频响应失真进行校正。并采用高通数字滤波的方法,修正加速度图的零线.为此编制了计算机程序,绘制了修正后的加速度、速度和位移时程曲线.计算了修正前后加速度图的傅氏谱。同时,对这些结果加以讨论。 修正后的加速度图,精确地表示了仪器基本频带在0.09HZ和25HZ之间的绝对地面加速度。   相似文献   

2.
用经验格林函数法模拟断层破裂过程,合成近场地面运动,并通过合成结果和真实记录的时程曲线、反应谱、傅氏谱的对比,估计断层破裂模型。  相似文献   

3.
在北京工业大学振动台台阵系统上开展了一系列锯末混合土地基自由场振动台模型试验,试验中模型箱采用装配式连续体刚性模型箱,试验中输入地震动时程采用El Centro地震动记录、Taft地震动记录和天津地震动记录,地震动输入方向分为水平单向和水平双向。文中,重点考察了双向地震动输入下锯末混合土模型场地的动力特性及其变化规律,主要指标包括模型场地地震动反应的峰值加速度及其动力放大系数、加速度时程及其傅氏谱。试验结果表明:随着输入地震动强度的增大,同一测点反应的峰值加速度总体上在增大,而其加速度动力放大系数总体上呈现减小的趋势,反应的频谱组成从较高频率向较低频率移动;双向地震作用下锯末混合土模型场地的动力变化规律与单向地震作用下较为一致。  相似文献   

4.
考虑相位谱的人造地震动反应谱拟合   总被引:34,自引:7,他引:34  
本文在回顾了地震动模拟理论及反应谱拟合技术的发展后,提出了一个新的加速度时程曲线的拟合方法,以改进现有反应谱拟合精度和原则。此法不同于常规方法之处有二:(一)在对幅值谱修正时,考虑了傅氏谱各分量对最大反应贡献的正负;(二)对于仅用幅值谱修正不能满足要求的顽固点,提出了相位修正的方法。这一力法使拟合技术更为合理而有效。  相似文献   

5.
根据台站场地条件进行地震动参数校正,有助于提高地震预警的有效性和准确性。针对我国地震预警台网中部分台址场地条件信息不完整及观测仪器的多样性,通过采用不同灵敏度的力平衡式加速度仪、速度仪和MEMS烈度仪,同时进行大量不同类别场地的地脉动观测,多角度对比分析时、频差别,探讨基于地震预警仪观测地脉动评价场地条件的可行性。结果表明,加速度仪灵敏度越高,H/V谱比卓越频率越易识别;速度仪与力平衡式加速度仪观测的地脉动,三分向傅氏谱和H/V谱比的谱形与卓越频率均一致;与TAG-33M强震仪相比,TMA-53烈度仪观测的地脉动整体幅值略高,波形较差,但随着振幅增大趋于一致;在近80%的场地上,TAG-33M强震仪与TMA-53烈度仪观测的地脉动傅氏谱卓越频率相差<0.5 Hz;当幅值均方根值>0.05 Gal时,TAG-33M强震仪与TMA-53烈度仪观测的地脉动竖向和水平向傅氏谱均趋于一致;当幅值均方根值为0.02 Gal~0.05 Gal时,TAG-33M强震仪与TMA-53烈度仪观测的地脉动竖向和水平向傅氏谱谱形均有较高的相似性;当幅值均方根值<0.02 Gal时,TAG-33M强震仪与TMA-53烈度仪观测的地脉动傅氏谱谱形相差较大,相似性低;依据TAG-33M强震仪观测地脉动H/V谱比的卓越频率判定场地类别,准确率达83.3%;TMA-53烈度仪观测地脉动的H/V谱比过于平坦,大多数场地上卓越频率识别困难。  相似文献   

6.
土-地铁车站结构动力相互作用大型振动台模型试验研究   总被引:12,自引:5,他引:12  
以南京地铁为背景,开展了深厚软弱场地土-地铁地下结构动力相互作用的大型振动台模型试验研究。在试验中获得的主要数据有:模型体系的加速度反应时程、模型结构的应力反应时程和结构表面的土压力时程等。本文对试验反映的地铁车站结构的动力反应规律及其周围模型地基的地震反应规律进行了分析。结果表明:车站结构的中柱应变反应明显大于别的构件,同时,深厚软弱地基上车站结构侧墙底部的应变反应也明显大于侧墙顶部的反应,其中,车站结构顶板、中间层楼板和底板的应变反应都很小;输入地震动的频谱特性对车站结构应变反应的影响是不同的,在同一加载情况下,在台面输入傅氏谱频宽最大的南京人工波时车站结构应变反应最大。  相似文献   

7.
陶夏新  王国新 《地震学报》2003,25(2):191-198
为了模拟近场强地震动,采用了基于有限断层模型的一种随机合成方法.震源破裂面被剖分成一定数量的子源,总的地震矩分成数量更多的子震的矩.一给定子源中一次子震引起的场地地震动的傅氏谱,通过考虑点源的谱、随着距离的衰减、能量耗散及近地表效应等导出.据此幅值谱和一个随机相位谱,并与一个时程包络函数结合,合成一个子震时程.将各子源中各个子震引起的所有时程叠加,得出场地的地震动时程.叠加中,各子震时程之间的时滞,据子震发震时差和子源至场地的距离差别引起的时差确定.对一个设定地震,选用4个断层面倾角,计算了近场21个地点的地震动.结果表明,本文方法可以很好地表达破裂的方向性效应和上盘效应.为了验证方法的可靠性,对1994年美国北岭地震中3个近断层台站MCN,LV3和PCD模拟的地震动与实际记录的加速度反应谱和时程作了比较.   相似文献   

8.
本文针对我国强震台网所普遍使用的电流计记录式强震仪和模拟记录数字化设备的特点,系统、全面地分析了数字强震加速度记录中包含的各类误差的性质和特点,在这样基础上给出的调整(未校正)加速度记录、校正加速度记录以及各类反应谱和傅氏谱的结果具有统一的精度和标准的格式.从而可以在相当广泛的范围内满足地震工程研究对常用地震动数据处理和分析的需要.   相似文献   

9.
1962年3月19日新丰江水库大坝附近发生MS 6.1级强烈地震后,13-17#坝段在108.5m高程处出现了长达82m的贯穿裂缝,导致水库渗漏,其后虽进行了加固处理,但经过50多年的运营,贯穿裂缝的现状如何,备受各级政府及专家学者的关注。本文利用近些年大坝上的多次小震观测记录,通过对有无贯穿裂缝坝段的地震加速度时程傅氏谱及上下坝体传递函数的对比分析,对14#坝段的整体性和稳定性进行了系统研究。结果表明,到目前为止,大坝贯穿裂缝没有明显恶化,但整体性依然较差,仍然是大坝稳定性的最大隐患。  相似文献   

10.
文献〔1〕介绍了局部加密的傅氏谱的算法。本文阐明了其基本思想和主要步骤并给出一个实用的计算程序和算例,供有关人员参考。  相似文献   

11.
The 2015 Illapel earthquake produced self‐evacuation of tall buildings in the city of Buenos Aires, Argentina, located 1280 km away from the epicenter. The ground motions in Buenos Aires due to the main event (Mw 8.3) and its aftershocks were registered by a new seismometer. The data collected allowed to estimate the maximum story drift ratios and top floor accelerations for tall buildings in Buenos Aires. The similarities between the response spectra and the Fourier amplitude spectra for the mainshock and its aftershocks show the influence that the dynamic properties of the 300‐m soil deposit have on the large acceleration amplification produced in these groups of buildings.  相似文献   

12.
地铁运行产生的环境振动超过一定值会影响人体健康,准确评价地铁运行引起的振动响应值意义重大。本文采用进口测振仪分别对青岛地铁3号线和上海地铁10号线进行现场测振,对数据进行处理得出振动加速度时程曲线,对测试数据进行Fourier变换得到相应的频谱曲线,将频谱曲线按1/3倍频程滤波转化为1/3倍频程谱,进而计算出分频振级平均值。通过加速度时程、频谱、1/3倍频程谱和分频振级的对比分析,结果表明:青岛地铁振动响应明显大于上海地铁,其分频振级已超过我国的环境振动标准,而上海地铁的分频振级基本上与我国的环境振动标准相当。  相似文献   

13.
Studies on the effect of near-surface overburden soil layers on seismic motion have shown that the overburden soil layers have a significant impact on the seismic effect of the site due to the formation age, genetic type, thickness difference, structure, and dynamic characteristics of the soil layers. In this paper, the one-dimensional seismic response analysis of a nuclear power plant site containing a thick hard interlayer was conducted to discuss the influence of the hard interlayer thickness on the site seismic response, so as to provide a basis for determining the seismic motion parameters for seismic design of similar sites. Based on the engineering geological data of a nuclear power plant site, five models of one-dimensional soil-layer seismic response analysis were built, and the equivalent linear method of the one-dimensional site seismic response was applied to analyze the effect of the interlayer thickness on the peak acceleration and the acceleration response spectra of the site seismic response. The seismic response characteristics of the site and influence rules of the hard interlayer thickness are summarized as follows:1)Under different input seismic motion levels, the peak acceleration at the top of the hard interlayer was less than the input peak acceleration, and the peak acceleration at the ground surface of site was greater than the input peak acceleration. 2)Under the same input seismic motion, the ratios of the peak accelerations at the top of hard interlayer to the input peak accelerations were smaller than the ratios of the peak accelerations at the ground surface to the input peak acceleration, and these ratios first decreased and then increased gradually with the increase of the hard interlayer thickness; while for the same hard interlayer thickness, these ratios gradually decreased as the input peak acceleration increasing. 3)For the same input seismic motion, the ratios of the peak accelerations at the ground surface of site to those at the top of the hard interlayer increased gradually as the hard interlayer thickness increased; however, corresponding to different hard interlayer thicknesses, the variation characteristics of ratios which are the peak accelerations at the ground surface of site to those at the top of the hard interlayer were inconsistent with the increase of the input peak acceleration. 4)The hard interlayer had a significant influence on the short-period acceleration response spectrum and the thicker the hard interlayer was, the wider the influence frequency band would be; while for a special hard interlayer thickness, the influence frequency band is certain, and the hard interlayer had little effect on the acceleration response spectrum coordinates outside this frequency band, the longer the period is, the less the influence of the hard interlayer on the acceleration response spectrum coordinates. The seismic response characteristics of the site and influence rules of the hard interlayer thickness indicate that the hard interlayer thickness has a significant impact on the peak acceleration and the acceleration response spectra of the site seismic response, and the hard interlayer has obvious isolation effect at the seismic motion, and the increase of its thickness reduces the nonlinear effect of the site and leads to the wider influence frequency band. Meanwhile, the higher the input peak acceleration is, the stronger the nonlinear effect of the site, and it's remarkable that the soft layer overlying the hard interlayer has a significant amplification effect on the seismic motion.  相似文献   

14.
汶川地震强地面运动模拟   总被引:3,自引:0,他引:3       下载免费PDF全文
常莹  周红  俞言祥 《地震学报》2012,34(2):224-234
基于确定性震源模型的方法主要用于计算低频(11 Hz)地震动常用经验格林函数法或随机方法,对低频地震动模拟不够准确.本文在确定性震源模型方法基础上,尝试采用分解给定的震源模型的方法来模拟宽频带(0.1——10 Hz)强地面运动,即采用分级离散断层面和分解断层面破裂单元上升时间的方法,增加震源时间函数中的高频信号,从而避免了对地震记录丰富程度和准确性的依赖.文中模拟计算了汶川MS8.0地震在8个地震观测台的地震动,将模拟结果和观测记录进行了加速度时程曲线和傅里叶振幅谱的对比分析.对比结果显示,模拟估计的地震动峰值加速度和持续时间与观测记录的数据基本在plusmn;50%的精度范围内相同,傅里叶振幅谱显示模拟结果有得到10 Hz左右的高频成分. 四川盆地中的台站模拟结果高频衰减比观测记录要快,原因是模拟过程没有考虑场地效应.对强地震动模拟还是要综合考虑震源、传播路径和场地的影响.研究结果表明,此改变震源输入的确定性方法可应用于模拟近断层宽频强地面运动.   相似文献   

15.
This paper attempts to show analytically that the energy-input spectra of damped SDOF systems and undamped MDOF systems excited by an earthquake motion can be predicted by smoothing the Fourier amplitude spectrum of the base acceleration. The spectral window for smoothing in the frequency domain for a damped SDOF system is identical with the probability density function of the time-variant or instantaneous vibration frequency resulting from non-linear hysteresis. The spectral window for an undamped MDOF system is identical with the set of squared participation factors associated with vibration modes. It was found that the increase in damping factor and the increase in participation of higher modes provide wider spectral windows, resulting in more flattened or unaltered energy-input spectra due to enhanced smoothing effects.  相似文献   

16.
Most acceleration diagrams show high levels of unpredictability, as a result, it is the best to avoid using diagrams of earthquake acceleration spectra, even if the diagrams recorded at the site in question. In order to design earthquake resistant structures, we, instead, suggest constructing a design spectrum using a set of spectra that have common characteristics to the recorded acceleration diagrams at a particular site and smoothing the associated data. In this study, we conducted a time history analysis and determined a design spectrum for the region near the Lali tunnel in Southwestern Iran. We selected 13 specific ground motion records from the rock site to construct the design spectrum. To process the data, we first applied a base-line correction and then calculated the signal-to-noise ratio (RSN) for each record. Next, we calculated the Fourier amplitude spectra of the acceleration pertaining to the signal window (1), and the Fourier amplitude spectra of the associated noise (2). After dividing each spectra by the square root of the selected window interval, they were divided by each other (1 divided by 2), in order to obtain the RSN ratio (filtering was also applied). In addition, all data were normalized to the peak ground acceleration (PGA). Next, the normalized vertical and horizontal responses and mean response spectrum (50%) and the mean plus-one standard deviation (84%) were calculated for all the selected ground motion records at 5% damping. Finally, the mean design spectrum and the mean plus-one standard deviation were plotted for the spectrums. The equation of the mean and the above-mean design spectrum at the Lali tunnel site are also provided, along with our observed conclusions.  相似文献   

17.
傅磊  李小军 《地球物理学报》2017,60(8):2935-2947
在地震动模拟中,高频衰减参数(κ0)是一个重要的参数,它控制了傅里叶谱高频部分的衰减特性.本文利用汶川MS8.0地震和芦山MS7.0地震主余震的1671组强震动观测记录,计算了龙门山地区50个断层距小于150 km的强震动台站的κ0,基于随机有限断层法模拟了汶川地震中这些台站的加速度时程、傅里叶振幅谱和反应谱,并与前人的研究进行比较.结果表明,合理计算的κ0可以有效地改善加速度时程振幅和高频谱(>1 Hz)的模拟结果.另一方面,本文基于κ0与地形高程的相关性,建立了龙门山地区的κ0经验模型.分别采用该经验模型和κ0= 0.04 s模拟了汶川地震的峰值加速度分布,并与观测记录进行比较.结果表明,采用本文提出的κ0模型可以更好地重现汶川地震的峰值加速度分布,特别是在断层破裂方向的反方向区域和山区.综上,汶川地震中山区的峰值加速度明显大于盆地地区的现象,不仅与断层破裂产状有关,还与山区和盆地地区的κ0之间显著的差异有关.  相似文献   

18.
2008年汶川MS8.0地震中, 固定和流动地形影响台阵记录到大量主余震记录, 本文通过对其均方根加速度、 相对持时、 频谱等要素进行分析, 讨论了山体地形效应的特征及其影响因素. 对于自贡西山公园地形台阵各测点的分析结果显示: 该台阵山脚基岩位置地震动的均方根加速度和相对持时明显低于山体周边土层场地和山体基岩测点; 随着高程的增加, 山体基岩测点的均方根加速度逐渐变大, 相对持时则变化不大, 傅里叶谱形状也大体一致, 在2.0—5.0 Hz频段内有所放大; 山体周边土层场地和山体地形对于相同地震动输入中不同频段内地震动能量的放大水平不同, 从而导致二者的地表地震动强度产生显著差异, 且前者对地震动持时的增加更加显著.   相似文献   

19.
基于HHT的结构强震记录分析研究   总被引:5,自引:0,他引:5  
本文利用HHT(Hilbert-HUang Transform)研究了结构强震记录的时频特性及结构动力特性。介绍了一座7层钢混框架结构及其强震观测台阵概况以及经历的地震情况,选择了在3次有代表性地震中的强震记录,利用一种新的非平稳信号处理方法HHT对记录进行了处理和分析,得到了该结构强震记录的时频幅值三维分布以及边际谱,并将边际谱与傅里叶谱进行了对比,识别了结构的自振频率。研究表明,对结构强震记录这种强非平稳信号,可以利用HHT分析得到能量集中分布的频段与时间范围。HHT边际谱与傅里叶谱相比,在低频部分幅值要大于傅里叶谱,而在高频部分,幅值要小于傅里叶谱。利用结构强震记录识别的自振频率比环境振动测试结果要小。  相似文献   

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