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1.
印尼附近海域地震海啸发生的构造背景综述   总被引:3,自引:0,他引:3  
2004年12月26日在印度尼西亚苏门答腊岛以西海域发生的里氏9级地震,引发了历史上第五大地震海啸,引起了地学界的高度关注。印度尼西亚西部位于环太平洋地震带和地中海-喜马拉雅地震带结合部位,处于洋壳和陆壳的汇聚边界以及弧状压缩构造格局中。苏门答腊陆缘NW—SE向延伸约1600km,苏门答腊俯冲带源于印度-澳大利亚和欧亚板块3°N的汇聚。苏门答腊弧前区沿着平行于俯冲海沟的两大走滑断裂——苏门答腊大断裂和明打威断裂向北运动。本文对印度尼西亚苏门答腊岛附近海域的地质背景、大地构造特征和地震活动评估等进行了综述,对该海域产生大地震的深部动力学机制进行了分析,并从地质、地球物理资料的获取与分析角度出发,对区域灾害模型进行了探讨。  相似文献   

2.
Tsunami hazard in the Makran Subduction Zone (MSZ), off the southern coasts of Iran and Pakistan, was studied by numerical modeling of historical tsunami in this region. Although the MSZ triggered the second deadliest tsunami in the Indian Ocean, among those known, the tsunami hazard in this region has yet to be analyzed in detail. This paper reports the results of a risk analysis using five scenario events based on the historic records, and identifies a seismic gap area in western Makran off the southern coast of Iran. This is a possible site for a future large earthquake and tsunami. In addition, we performed numerical modeling to explain some ambiguities in the historical reports. Based on the modeling results, we conclude that either the extreme run-up of 12–15 m assigned for the 1945 Makran tsunami in the historical record was produced by a submarine landslide triggered by the parent earthquake, or that these reports are exaggerated. The other possibility could be the generation of the huge run-up heights by large displacements on splay faults. The results of run-up modeling reveal that a large earthquake and tsunami in the MSZ is capable of producing considerable run-up heights in the far field. Therefore, it is possible that the MSZ was the source of the tsunami encountered by a Portuguese fleet in Dabhul in 1524.  相似文献   

3.
林法玲 《台湾海峡》2012,31(4):565-570
福建地处西北太平洋沿岸,在环太平洋地震带附近,是海啸灾害潜在风险区."3.11"日本地震海啸,福建沿岸验潮站就监测到其海啸波.利用CTSU地震海啸数值模式,模拟了"3.11"日本地震海啸对福建近海的影响,模拟结果与实况较吻合.同时,利用该数值模式模拟分析了可能来自于琉球群岛和南海附近海域的地震海啸对福建近海的影响,分析表明,如果在琉球群岛海域(28.0°N,129.0°E)发生8.8级地震,引发的海啸波将在4.5 h左右抵达福建北部海岸,最大海啸波幅可达2 m;如果在马尼拉海沟附近海域(17.5°N,119.0°E)发生8.8级地震,引发的海啸波将在4 h左右抵达福建南部海岸,最大海啸波幅可达3 m,均会给福建沿海地区带来灾害性影响.为此,本文亦针对性提出了防范地震海啸的一些措施与建议,为福建省海洋防灾减灾提供参考.  相似文献   

4.
2015年9月16日22时54分(当地时间)智利中部近岸发生Mw8.3级地震,震源深度25 km。同时,强震的破裂区长200 km,宽100 km,随之产生了中等强度的越洋海啸。海啸影响了智利沿岸近700 km的区域,局部地区监测到近5 m的海啸波幅和超过13 m的海啸爬坡高度。太平洋区域的40多个海啸浮标及200多个近岸潮位观测站详细记录了此次海啸的越洋传播过程,为详细研究此次海啸近场及远场传播及演化规律提供了珍贵的数据。本文选择有限断层模型和自适应网格海啸数值模型建立了既可以兼顾越洋海啸的计算效率又可以实现近场海啸精细化模拟的高分辨率海啸模型。模拟对比分析了海啸的越洋传播特征,结果表明采用所建立的模型可以较好地再现远场及近场海啸特征,特别是对近场海啸的模拟结果非常理想。表明有限断层可以较好地约束近场、特别是局部区域的破裂特征,可为海啸预警提供更加精确的震源信息,结合高分辨率的海啸数值预报模式实现海啸传播特征的精细化预报。本文结合观测数据与数值模拟结果初步分析了海啸波的频散特征及其对模型结果的影响。同时对观测中典型的海啸波特征进行的简要的总结。谱分析结果表明海啸波的能量主要分布在10~50 min周期域内。这些波特征提取是现行海啸预警信息中未涉及,但又十分重要的预警参数。进一步对这些波动特征的详细研究将为海啸预警信息及预警产品的完善提供技术支撑。  相似文献   

5.
海啸灾害与预警   总被引:6,自引:0,他引:6  
地震海啸是最严重的自然灾害之一。本文对海啸的定义、性质、特征、历史上和近代的中国和世界的严重地震海啸灾害作了介绍。同时简单地介绍了海啸预警系统的主要内容。  相似文献   

6.
基于数值模拟的渤海海域地震海啸危险性定量化研究   总被引:1,自引:1,他引:0  
根据地震海啸产生的条件,结合渤海海域的地形特征、地质构造、地震学特征和历史地震及海啸记录对渤海海域潜在的地震海啸进行了数值模拟研究。分析了渤海可能引发地震海啸的震源区域,讨论了渤海发生海啸灾害的可能性。文中通过数值模拟再现了渤海历史上几次规模较大的地震事件可能引发的海啸情景,研究分析了可能的地震海啸在渤海及周边海域的传播过程及波动特征.地震海啸传播模型采用基于四叉树原理的自适应网格加密技术,有效解决了局部分辨率与计算效率之间的矛盾。数值计算包括地震海啸产生及传播过程。利用该模型对渤海潜在的地震海啸进行了数值计算,基于数值计算结果定量阐述了渤海海域潜在地震海啸对渤海局部岸段及北黄海沿岸的影响,给出了渤海可能地震海啸危险性划分;研究结果将为我国海啸危险性分析和海啸预警技术研究工作提供技术支持。  相似文献   

7.
A study of tsunami events in the East (Japan) Sea using continuous Galerkin finite element model, aiming at reproducing tsunami waves generated by underwater earthquakes in 1983 and 1993 respectively has been performed focusing on the geographic extent of a topographic feature in the East (Japan) Sea. Numerical models can be the proper tools to study the combined effects of realistic topography. Subsequently, using the FEM based two-dimensional model we have simulated the smoothed and flattened topographic effects by removal of Yamato Rise and seamounts for the cases of tthe 1983 Central region earthquake tsunami and the 1993 southwestern Hokkaido earthquake tsunami. The results have shown that there will be higher tsunamis along the eastern coasts of Korea in general except some areas, like Sokcho with removal of topographic highs, thus providing complicated bottom topography of the East (Japan) Sea as effective tsunami energy scattering.  相似文献   

8.
2017年9月8日4时49分(UTC),墨西哥瓦哈卡州沿岸海域(15.21°N,93.64°W)发生Mw8.2级地震,震源深度30 km。强震在该海域引发海啸,海啸对震源附近数百千米范围内造成了严重影响。位于太平洋上的多个海啸监测网络捕捉到了海啸信号并详细记录了此次海啸的传播过程。本文选用了近场2个DART浮标和6个验潮站的水位数据,通过潮汐调和分析和滤波分离出海啸信号,对近场海啸特征值进行了统计分析,并采用小波变换分析方法进一步分析了海啸的波频特征。基于Okada弹性位错理论断层模型计算得到了强震引发的海底形变分布,并采用MOST海啸模式对本次海啸事件近场传播特征进行了模拟,模拟结果与观测吻合较好。最后,基于实测和模拟结果,详细分析了此次地震海啸的近场分布特征,发现除受海啸源的强度和几何分布特征影响外,近岸海啸波还主要受地形特征控制,在与特定地形相互作用后波幅产生放大效应,会进一步加剧海啸造成的灾害。  相似文献   

9.
For a long time, people have believed that the vertical displacement of seafloor due to undersea earthquakes is the primary cause of tsunami genesis. However, seismically-inverted seafloor deformation of the 2004 Sumatra–Andaman earthquake shows that the total vertical displacement is not enough to have generated the powerful Indian Ocean tsunami. Based on the seismically-inverted data and a three-dimensional ocean general circulation model (OGCM), we show that the momentum force, transferred by the horizontal impulses of the faulting continental slope in that earthquake, has accounted for two thirds of the satellite-observed tsunami height and generated kinetic energy 5 times larger than the potential energy due to the vertical displacement. The asymmetric tsunami pattern, recorded by tide-gauges showing leading-elevation waves toward Sri Lanka and leading-depression waves toward Thailand, is best explained by the horizontally-forced mechanism. The same mechanism has also explained the March 2005 Nias earthquake and tsunami data, suggesting that the horizontal motions of faulting have played more important roles in tsunami genesis than previously thought.  相似文献   

10.
On February 6th, 1783, a landslide of about 5 × 10m3 triggered by a 5.8 M earthquake occurred near the village of Scilla (Southern Calabria, Italy). The rock mass fell into the sea as a rock avalanche, producing a tsunami with a run-up as high as 16 m. The tsunami killed about 1,500 people, making it one of the most catastrophic tsunamis in Italian history. A combined landslide-tsunami simulation is proposed in this paper. It is based on an already performed reconstruction of the landslide, derived from subaerial and submarine investigation by means of geomorphological, geological and geomechanical surveys. The DAN3D model is used to simulate the landslide propagation both in the subaerial and in the submerged parts of the slope, while a simple linear shallow water model is applied for both tsunami generation and propagation. A satisfying back-analysis of the landslide propagation has been achieved in terms of run-out, areal distribution and thickness of the final deposit. Moreover, landslide velocities comparable to similar events reported in the literature are achieved. Output data from numerical simulation of the landslide are used as input parameters for tsunami modelling. It is worth noting that locations affected by recordable waves according to the simulation correspond to those ones recorded by historical documents. With regard to run-up heights a good agreement is achieved at some locations (Messina, Catona, Punta del Faro) between computed and real values, while in other places modelled heights are overestimated. The discrepancies, which were most significant at locations characterized by a very low slope gradient in the vicinity of the landslide, were probably caused by effects such as wave breaking, for which the adopted tsunami model does not account, as well as by uncertainties in the historical data.  相似文献   

11.
文中利用在有限体积近海模型FVCOM基础上拓展开发的全球海洋模型GOCTM(Global Ocean Circulation and Tide Model)进行了海啸波传播过程模拟,GOCTM采用全球无结构三角形网格,避免了开边界条件引入带来的误差,利用德国AWI研究所提供的海啸源作为初始水位场,模拟了2004年12月26日苏门答腊-安达曼Mw 9.2地震引发的海啸传播过程。通过模拟结果与印度沿岸潮位站数据以及海啸发生过程观测到的卫星高度计数据进行了对比,发现模拟结果与观测值相近,相关系数最高达0.82,相关性较好。模拟的海啸波到达苏门答腊岛北部的时间与日本的TUNAMI 模型和德国AWI研究所的TsunAWI模型的模拟结果相符,时间相差不到30 min,证明GOCTM全球模型可以较好地对海啸传播过程进行模拟,结果令人满意,希望本工作可以为我国海啸预报和预警提供参考。  相似文献   

12.
2011年3月11日日本宫城县以东太平洋海域发生Mw9.0级特大地震,造成了地表的严重错位并引发海啸。文中利用位于日本及周边国家的IGS站和国家海洋局GPS业务站观测数据,采用作者研制的精密单点定位(PPP)软件UniP,对此次地震的GPS数据响应进行了研究。结果表明:(1)GPS观测数据能清晰、连续地记录震时地表形变的过程,我国CHAN,NCST等站点水平方向的震时最大位移在10 cm以内,高程方向的震时最大位移在15 cm以内,且形变以可恢复性的弹性形变为主。(2)我国距震中较远,受此次日本地震的影响较小,且大部分站点是在东坐标方向出现不同程度的震后永久性位移。其中CHAN站点的震后位移最为明显,东向形变量为(1.8±0.11)cm;NCST、NLHT站点次之,东向形变量分别为(1.1±0.26)cm和(1.0±0.18)cm。(3)地震波传输到国家海洋局GPS业务站NCST、NLHT等的时间约为10 min,比海啸在深海的传播速度快约14倍,可为海啸预警提供所需的时间差。这些结果显示出GPS能够为地震监测和动力学特征研究提供有价值的基础资料,也表明中国沿海GPS业务观测系统在海底地震监测、海啸预警服务中的应用潜力。  相似文献   

13.
浅水方程被广泛应用于海啸预警报业务及研究,而针对线性浅水方程与非线性浅水方程在不同海区水深地形条件下的适用范围、计算效率问题是海啸研究人员急需了解的。本文应用基于浅水方程的海啸数值预报模型就海啸波在南海、东海传播的线性、非线性特征以及陆架对其传播之影响进行了数值分析研究。海啸波在深水的传播表征为强线性特征,此时线性系统对海啸波幅的模拟计算具有较高的精度和效率,而弱的非线性特征及弱的色散特征对海啸波幅的预报影响甚微,可以忽略不计。海啸波传播至浅水大陆架后受海底坡度变化、海底粗糙度等因素影响,波动的非线性效应迅速传播、积累,与线性浅水方程计算的海啸波相比表现出较大差异,主要表现为:在南海区,水深小于100m时,海啸波首波以后的系列波动非线性特征比较明显,两者波幅差别较大,但首波波幅的区别不大,因此对于该区域在不考虑海啸爬高的情况下,应用线性系统计算得到的海啸波幅也可满足海啸预警报的要求;在东海区由于陆架影响,海啸波非线性特征明显增强,水深小于100m区域,首波及其后系列波波幅均差异较大,故在该区域必须考虑海啸波非线性作用。本文就底摩擦项对海啸波首波波幅的影响进行了数值对比分析,结果表明:底摩擦作用对海啸波首波波幅影响仅作用于小于100m水深。最后,该文通过敏感性试验,初步分析了陆架宽度及陆架边缘深度对海啸波波幅的影响,得出海啸波经陆架传播共振、变形后,海啸波幅的放大或减小与陆架的宽度及陆架边缘水深有关。  相似文献   

14.
海啸波对近岸岛礁影响的数值模拟研究   总被引:1,自引:0,他引:1  
基于Okada有限断层模型和非线性浅水波方程,结合高精度嵌套网格建立了越洋(中国近海)-局部-近岸岛礁的海啸生成与传播的数值模型。以三亚凤凰岛为例,首先针对2011日本地震海啸,模拟分析了海啸波沿中国沿海大陆架的传播特征及对凤凰岛的影响规律。在取得验证结果的基础上,进一步讨论了中国近海的马尼拉海沟和琉球海沟的潜在海啸源,以及环太平洋的21个潜在特大越洋海啸对凤凰岛的影响特征。依据海啸波在抵达凤凰岛的波浪特征,结合傅里叶频谱分析方法,探索了近岸岛礁对海啸波的放大效应。结果表明,中国近海一般震级的海啸和特大越洋海啸对凤凰岛存在一定影响,最大波幅接近1 m,传播时间从3 h到27 h不等。受三亚东南半岛的影响,琉球海沟激发的海啸和越洋海啸在凤凰岛的放大效应相对于马尼拉海沟较小,其频率集中在0.8×10-4~2×10-4 Hz。马尼拉海沟产生的海啸波在凤凰岛产生了较为显著的放大效应,对于凤凰岛是值得关注的高风险海啸源。  相似文献   

15.
越洋海啸的数值模拟及其对我国的影响分析   总被引:7,自引:2,他引:5  
简要介绍了地震海啸产生的物理机制、海啸波在大洋中的传播特性以及海啸所具有的超强破坏力可能引发的巨大灾害;概述了全球地震海啸发生的频率和太平洋区域历史海啸的时空分布;整理分析了我国沿海发生海啸的频次和空间分布。针对越洋海啸传播的特点,采用基于波浪追逐原理和自适应网格加密技术的海啸数值模型对1960智利海啸进行了数值模拟,将模拟的结果与历史记录进行了对比,验证了模型的可靠性。通过对数值模拟结果的分析,初步讨论了我国沿海地区越洋海啸的危险性,并定量阐述了越洋海啸对我国各海区的影响。  相似文献   

16.
深圳海域潮汐海啸波耦合数值研究   总被引:3,自引:0,他引:3  
以COMCOT海啸模式和TPXO7.1全球潮汐模式为基础,采用三层嵌套网格,建立了南海海啸与潮汐耦合计算模型,分析深圳海域海啸和潮汐相互作用。潮汐计算结果与实测数据吻合较好,高、低潮位平均误差小于15 cm,20 cm;在潮汐验证的基础上,以马尼拉海沟潜在地震海啸源为案例,进行8.0,9.0级地震海啸与潮汐耦合情景模拟计算,计算结果表明,9级地震海啸在深圳海域外海波高为140~150 cm,如先行波为正波发生在高潮时将产生异常高潮位,负波发生在低潮时将产生异常低潮位,线性叠加计算结果偏大,在25.0 cm之内,到达时间差异小于6 min。  相似文献   

17.
The “seismic silence” period in the seismic gap in the region of the Komandor Islands (hereinafter, the Komandor seismic gap) is close to the duration of the maximal recurrence interval for the strongest earthquakes of the Aleutian Islands. This indicates the possibility of a strong earthquake occurring here in the nearest time. In the present work, the results of simulation for a tsunami from such an earthquake are presented. The scheme successfully used by the authors for the nearest analog—the 2004 Sumatra-Andaman earthquake—is applied. The magnitude of the supposed earthquake is assumed to be 9.0; the tsunamigenic source is about 650 km long and consists of 9 blocks. The parameters of the tsunami propagation in the Pacific Ocean and the characteristics of the waves on the coasts are computed for several possible scenarios of blocks’ motion. The spectral analysis of the obtained wave characteristics is made and the effects of the wave front interference are found. Simulation has shown that the wave heights at some coastal sites can reach 9 m and, thus, may cause considerable destruction and deaths.  相似文献   

18.
The tsunami which follows a strong local earthquake occurs within a few minutes of the origin time. This requires that any warning system for such local tsunamis be decentralized, as in the system used by the Japan Meterological Agency. Thus, decisions are being made by local officials rather than in a central office. This usually means that the level of training, the education, and the preparation is not as intense in such a local office as in a central office. Therefore, the decision making should be assisted by instrumentation that discriminates tsunamigenic earthquakes from non‐tsunamigenic earthquakes. This is not yet possible in real time; however, since only very large earthquakes (more than 6.5) generate significant tsunamis, an instrument to inform the local official of the tsunami prospects can be implemented.

An instrument for assisting the local decision maker has been developed. This instrument consists of an analog computer (an inverted pendulum having a period of 0.75 sec and damping about 0.3) and a digital computer (a hardwired signal‐recognition circuit), providing output to a display of status or alarm. The level of displacement (or velocity or acceleration) , the number of times that the threshold must be exceeded, and the time window within which the excedance must occur are all adjustable. Initial settings require about 0.06 g three times, not more than ten seconds apart. Battery back‐up and test circuitry are provided.

Since the operating instructions require that motion be felt before the instrument alarm be considered valid, great weight is given to assuring that the instrument will operate when required. The instru‐ment is always “ON,”; with the earthquake turning it “OFF”; thus, it is continually self‐testing.

Twelve units have been installed in police stations, fire stations, or similar locations around the State of Hawaii, which funded the system developed at Indiana University. This tsunami seismic trigger should be considered whenever the primary objective is to trigger an alarm rather than to record data; the emphasis in design and development has been on reminding the local official when there may be a tsunami hazard and not on recording research data.  相似文献   

19.
推导了地震海啸波传播的理论方程,并时局地地震海啸情况下的理论方程进行了求解.基于Boussinesq方程出发,建立了二维局地海啸渡传播数学模型;对局地海啸进行了数值计算,计算方法采用有限差分方法.差分格式采用交替方向隐格式,即ADI方法.利用该模型对发生在台湾海峡的一次地震海啸进行了模拟计算.将计算结果与理论方程的计算结果以及实际情况进行了对比.计算结果较好.为局地海啸波传播提供了一种模拟方法.  相似文献   

20.
《Marine Geology》2006,225(1-4):311-330
The MW = 7.4 earthquake that affected the northwestern part of Turkey on August 17, 1999, and in particular the gulf of İzmit, had dramatic consequences also as regards tsunami generation. The main cause of the earthquake was a dextral strike-slip rupture that took place along different segments of the western part of the North Anatolian Fault (WNAF). The rupture process involved not only a number of distinct strike-slip fault segments, but also dip-slip ancillary faults, connecting the main transcurrent segments. The general picture was further complicated by the occurrence of subsidence and liquefaction phenomena, especially along the coasts of the İzmit bay and in the Sapanca Lake. Tsunami effects were observed and measured during post-event surveys in several places along both the northern and the southern coasts of the bay. The run-up heights in most places were reported to lie in the interval 1–3 m: but in the small town of Değirmendere, where a local slump occurred carrying underwater buildings and gardens of the waterfront sector, eyewitnesses reported water waves higher than 15 m.The purpose of this work is to investigate on the causes of the tsunami by means of numerical simulations of the water waves. We show that the tsunami was a complex event consisting at least of the combination of a regional event due to tectonic causes and of a local event associated with the mass failure. As to the first, we are able to demonstrate that the observed tsunami cannot be explained only in terms of the sea bottom dislocation produced by the main right-lateral dislocation, but that the prominent contribution comes from the displacement associated with the secondary shallow normal faults. Furthermore, the large waves and effects seen in Değirmendere can be explained as the consequence of the slump. By means of a stability analysis based on an original method making use of the limit equilibrium concept, we show that the slump was highly stable before the earthquake and that it was triggered by seismic waves. Simulation of the tsunami induced by the slump was carried out by a two-step numerical code that computes the landslide motion first, and then the generated water wave propagation. It is shown that the computed local tsunami matches the experimental data.  相似文献   

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