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151.
最不利地震动在网壳结构抗震设计中的应用   总被引:3,自引:0,他引:3  
利用文献提供的最不利地震动,对网壳结构等大跨空间结构进行了分析,分别考察了仅水平输入和三向地震波输入的两种情况,对最不利地震动在网壳结构抗震设计中的适用性进行了探讨,并在一实际工程设计中进行了应用。大跨度空间结构在水平地震动输入时,宜按照的最不利地震动进行设计;在三向地震动同时输入时,应同时分别按所推荐最不利设计地震动和按常规选用的地震动,对大跨度空间结构进行抗震分析。  相似文献   
152.
介绍了地震信号传输的常用方式及各自的优缺点,提出了数字遥测地震台网信号传输方式设计的总原则和基本原则。实际应用表明,兰州数字遥测地震台网信号传输方式的是符合要求的,提出的数字遥测地震台网信号传输方式的总原则和基本原则,对数字遥测地震台网建设有直接的借鉴作用。  相似文献   
153.
就如何利用数据库,结合Java、XML等手段对震源参数管理进行了一些探索,并给出了一些在一个实际系统中实现了的例子。  相似文献   
154.
为使县级以上地震部门做好审核建设工程抗震设防要求工作,介绍了确定抗震设防要求的4个依据、程序、重大重要建设工程的划分依据、活动断裂分类与分级规定等。指出,确定抗震设防要求既是一项法定的行政审批工作,又是一项严谨的科学技术工作。  相似文献   
155.
设计了一种地震参数计算与数据传输程序,能够通过交互方式自动完成mb、mB、MS7、MS、ML五个震级及其他相关地震参数的计算,自动生成大震速报文件,直接连接PCU速报。不仅适用于数字地震仪同时也可以用于模拟仪器(如DD—1,DK—1)解决了SSB大震速报软件数据不易改动、容易出错、速度慢等问题。同时也完善了SSDP软件参数计算功能,提高了数字测震台的效能和速报水平,充分发挥了数字地震仪的优越性。  相似文献   
156.
海底MT信号采集电路的设计   总被引:11,自引:0,他引:11  
设计海底大地电磁信号采集电路,需考虑海底信号特征、海上作业以及海底环境等各种因素。分析表明,除遵循电路设计的一般原则外,海底大地电磁测量要重点解决微弱信号检测、智能化数据采集、海底环境监测和同步记录等4个方面的问题。在设计方案中,电路灵敏度达到微伏级;使用嵌入式计算机实现采集控制;对方位、倾斜、振动、温度等参数进行巡回记录;仪器的时钟精度精准到微秒。所研制的电路经过了室内模拟测试和海洋试验。首次采集到中国海域的大地电磁数据。  相似文献   
157.
Introduction An MS=6.0 earthquake occurred on February 23, 2001 in Yajiang county, Sichuan Province. The earthquake is located on the east of the southeast segment of the Litang-Dewu fault with strike of NW. Before the event, on February 14, an MS=5.0 earthquake took place nearly in the same place. In 1948 an MS=7.3 earthquake occurred on the northwestern segment of the Litang fault. The length of the surface rupture belt caused by the earthquake is 70 km, which extended from Litang to…  相似文献   
158.
1 Background of the new national seismic zoning map The policy of seismic disaster mitigation in the Chinese mainland is prevention first. According to the law, the earthquake design for ordinary structures must fit the demand of national seismic zoning map. Seismic zoning map is the basis of the earthquake design (TANG, 1998; WU, et al, 1998). The seismic zoning map must be updated with the progress in methodology and accumula-tion of the data. There are three generations of national seis…  相似文献   
159.
Tariq A. Khan   《Limnologica》2003,33(4):327-339
Major biological parameters of four permanent (Lake Colac, Modewarre, Bolac and Tooliorook), shallow and slightly saline lakes in the volcanic plains of western Victoria, Australia recorded bi-monthly between November 1999–September 2001 are described. Chlorophyll a concentration ranged from 3–29 μg l−1 with peaks in autumn. Phytoplankton taxa recorded were diverse, with Chlorophyta and Bacillariophyta being common. Cyanobacterial blooms were recorded mostly in summer. Zooplankton abundance in the lakes ranged from 12–368 individuals per litre. Rotifera dominated Lake Bolac, Copepoda dominated Lake Modewarre and they co-dominated Lake Colac and Tooliorook. Zooplankton interactions with phytoplankton suggest that simple predator-prey relationships cannot fully explain the trends exhibited and that a more complex model was acting to regulate algal biomass. A decline in the abundance of zooplankton in summer in Lake Modewarre was attributed to predation by high number of exotic larval carp at that time of the year. A total of 25 benthic macroinvertebrate taxa were recorded from Lake Colac, 30 from Modewarre, 22 from Bolac and 35 from Tooliorook. Twenty-one of the 45 taxa identified occurred in at least three lakes. Nine of the 12 taxa that occurred in only one lake were from Lake Tooliorook. Simpson's diversity index was low in Lake Bolac when compared to other three lakes. Lake Modewarre had more benthic individuals (3246 Ind m−2) than other three lakes (range 624–1397 Ind m−2). The combined contribution of Ostracoda, Amphipoda and Gastropoda dominated the benthos in all the lakes throughout the study period. Macroinvertebrate taxa richness was higher in the present study lakes than recorded from the lakes in the region. Frequency of sampling and number of sampling sites seemed more important in determining species richness than the size and shallowness of the lakes.  相似文献   
160.
The five MTMD models, with natural frequencies being uniformly distributed around their mean frequency, have been recently presented by the first author. They are shown to have the near‐zero optimum average damping ratio (more precisely, for a given mass ratio there is an upper limit on the total number, beyond which the near‐zero optimum average damping ratio occurs). In this paper, the eight new MTMD models (i.e. the UM‐MTMD1~UM‐MTMD3, US‐MTMD1~US‐MTMD3, UD‐MTMD1 and UD‐MTMD2), with the system parameters (mass, stiffness and damping coefficient) being, respectively, uniformly distributed around their average values, have been, for the first time here, proposed to seek for the MTMD models without the near‐zero optimum average damping ratio. The structure is represented by the mode‐generalized system corresponding to the specific vibration mode that needs to be controlled. Through minimization of the minimum values of the maximum dynamic magnification factors (DMF) of the structure with the eight MTMD models (i.e. through the implementation of Min.Min.Max.DMF), the optimum parameters and values of Min.Min.Max.DMF for these eight MTMD models are investigated to evaluate and compare their control performance. The optimum parameters include the optimum mass spacing, stiffness spacing, damping coefficient spacing, frequency spacing, average damping ratio and tuning frequency ratio. The six MTMD models without the near‐zero optimum average damping ratio (i.e. the UM‐MTMD1~UM‐MTMD3, US‐MTMD1, US‐MTMD2 and UD‐MTMD2) are found through extensive numerical analyses. Likewise, the optimum UM‐MTMD3 offers the higher effectiveness and robustness and requires the smaller damping with respect to the rest of the MTMD models in reducing the responses of structures subjected to earthquakes. Additionally, it is interesting to note, by comparing the optimum UM‐MTMD3 with the optimum MTMD‐1 recently investigated by the first author, that the effectiveness and robustness for the optimum UM‐MTMD3 is almost identical to that for the optimum MTMD‐1 (without inclusion of the optimum MTMD‐1 with the near‐zero optimum average damping ratio). Recognizing these performance benefits, it is preferable to employ the optimum UM‐MTMD3 or the optimum MTMD‐1 without the near‐zero optimum average damping ratio, when installing the MTMD for the suppression of undesirable oscillations of structures under earthquakes. Copyright © 2003 John Wiley & Sons, Ltd.  相似文献   
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