共查询到20条相似文献，搜索用时 163 毫秒
1.
安宁河-则木河-小江地震带强震危险性趋势讨论 总被引：1，自引：1，他引：0
研究了川滇地震区强震活动期格局的变化,认为自1976年以来已进入川滇地震区的"中区"为主体活动的新活跃期,并将可能持续至少二三十年;1985～1996年初的川滇强震活跃幕已经结束,1996～2002年处于6级地震的少发时段.根据川滇中区历史上出现过的东带(E102°～103°线)、西带(E100°线)交替活动特征估计未来几年安宁河-则木河-小江地震带将可能是大地震发生带. 相似文献
2.
3.
研究了东南沿海地震带20世纪第Ⅳ活跃幕的两个特征,包括该带中强地震与阳江地震窗的对应关系以及该带ML4地震长时间平静的震兆意义。结果表明:在第Ⅳ活跃幕中,阳江地区ML3地震(去余震)的活跃不仅与本区5级左右地震活动有关,还与东南沿海地震带5级以上强震活动有关,震前阳江地区ML3地震滑动3月频次出现升高现象,阳江地区ML3地震活动可作为东南沿海地震带的地震"窗口";在东南沿海地震带活跃幕期间,ML4地震发震间隔△T≥300d具有震兆意义,是5级地震的短期或中短期指标,而在平静幕期间,ML4地震的长时间平静并不具备震兆意义,只是区域应力场处于松弛状态下的正常表现。 相似文献
4.
应用灰色系统理论的关联分析方法研究了广西地震活动与我国主要地震区（带）地震活动的相关性．结果表明广西地震活动与东南沿海地震带地震活动的关联程度最大（ｒ＝０．８６）,根据这一结果,对广西与东南沿海地震带的地震活动的相关性作了进一步探讨,发现本世纪以来广西地震活动与东南沿海地震带的地震活动同步起伏,两区（带）之间发生中强地震的互相对应关系特别明显． 相似文献
5.
采用数理统计方法探讨了780 BC至今、100°—110°E、22°—35°N（中国南北地震带）区域的中国大陆5.0级及以上天然地震的分布规律。通过GMT软件绘制了南北地震带上地震震中和断裂分布图像，分析了南北地震带地震时空分布与地震活动性的规律。研究表明，该地区的大震与强震几乎全部发生在断裂带上，地震频次高、震中密集，呈现集群性等特征，地震活动性较高。该地震带中、南段相似，与北段存在显著差异。在南北地震带上，地震的活跃幕与平静幕持续时间，与活跃幕强度有关。研究结果对于了解地震的时空分布特征，认识中国南北地震带的发震规律，地震的孕震发震和地震活动周期有参考意义。 相似文献
6.
研究了1500年以来东南沿海地震区东部中强地震的活动特征。通过对其时序演变进程的分析,长乐-诏安地震带和邵武-河源地震带地震活动参数的对比,以及对第二活跃期中强地震迁移特点的研究,对该区今后的地震活动趋势作出了估计。 相似文献
7.
本活跃期以来山西地震带地震活动的基本特点 总被引：1，自引：0，他引：1
1815年平陆6~(3/4)级地震揭开了华北本活跃期的序幕,其后的175年中山西地震带虽未发生7级以上强震,但是中强地震频度较高。它们主要分布在大同-平陆北北东向剪切段内。时间序列的幕式活动特点和华北活跃幕的划分是一致的。应变释放速率显示了明显的加速现象。1989年大同-阳高6.1级地震的发生,进一步说明地震活动性的增强。本活跃期尚余的1～2个活跃幕中,山西地震带是值的注意的一个地区。 相似文献
8.
在北纬 2 1°～ 2 6° ,东经 119°～ 12 3°内 ,依据板块运动、地体构造界线、活动断层分析和强震震中分布四个因素 ,绘制台湾地区的地震地体构造区分图 ;将台湾地区分成东西两个地震区 ;E1～E4、W1～W4等共八个地震带。根据强震幕式分析、地震活动性水平分析、地震频次与缺震异常分析和空区与条带分析四个地震趋势分析步骤 ,分析 2 0 0 1年和 2 0 0 2年台湾地区的中强地震趋势。实际地震结果表明 ,这种地震趋势分析方法在台湾地区有非常好的应用效果。 相似文献
9.
淮河流域及南黄海中强地震区特征分析 总被引：1，自引：0，他引：1
淮河流域及南黄海地震区(29°—35°N,110°—123°E)在地壳深部结构、活动断层格局及新构造等方面具有由华北向华南过渡的特征。这些特征可能是形成中强地震区的重要构造背景条件之一。 该区地震活跃期和平静期的出现稍晚于华南地震区而又稍早于华北地震区,活跃期与平静期内的地震活动强度相差不很悬殊,活跃幕与平静幕的时间变化比较稳定。中强地震的时间间隔呈现重复的序列性特征,地震的经向、纬向分布表现出一百年左右的周期性变化。 相似文献
10.
11.
E.J. Delahaye J. Townend M.E. Reyners G. Rogers 《Earth and Planetary Science Letters》2009,277(1-2):21-28
Geodetically-detected episodes of slow slip appear in several subduction zones to be accompanied by bursts of low-frequency coherent noise known as seismic tremor, but whether a single physical process governs this association or even whether slow slip is invariably accompanied by tremor remains unresolved. Detailed analysis of broadband seismic data spanning a slow slip episode in the Hikurangi subduction zone, New Zealand, reveals that slow slip was accompanied by distinct reverse-faulting microearthquakes, rather than tremor. The timing, location, and faulting style of these earthquakes are consistent with stress triggering down-dip of the slow slip patch, either on the subduction interface or just below it. These results indicate that tremor is not ubiquitous during subduction zone slow slip, and that slow slip in subduction zone environments is capable of triggering high-frequency earthquakes near the base of the locked subduction thrust. In this and other locations (Hawaii, Boso Peninsula) where slow slip is accompanied by triggered microseismicity, the estimated upper extent of the slow slip is shallower (less than ~ 20 km) than in those locations from which tremor has been reported. This suggests that ambient temperature- or pressure-dependent factors govern the character of the seismic response to slow slip on subduction thrusts and other large faults, with rheological or lithological conditions at shallow depths triggering high-frequency microearthquakes and those at greater depths triggering seismic tremor. 相似文献
12.
The seismogenic zone of subduction thrust faults 总被引：13，自引：0，他引：13
Abstract Subduction thrust faults generate earthquakes over a limited depth range. They are aseismic in their seaward updip portions and landward downdip of a critical point. The seaward shallow aseismic zone, commonly beneath accreted sediments, may be a consequence of unconsolidated sediments, especially stable-sliding smectite clays. Such clays are dehydrated and the fault may become seismogenic where the temperature reaches 100--150°C, that is, at a 5--15 km depth. Two factors may determine the downdip seismogenic limit. For subduction of young hot oceanic lithosphere beneath large accretionary sedimentary prisms and beneath continental crust, the transition to aseismic stable sliding is temperature controlled. The maximum temperature for seismic behavior in crustal rocks is ～ 350°C, regardless of the presence of water. In addition, great earthquake ruptures initiated at less than this temperature may propagate with decreasing slip to where the temperature is ～ 450°C. For subduction beneath thin island arc crust and beneath continental crust in some areas, the forearc mantle is reached by the thrust shallower than the 350°C temperature. The forearc upper mantle probably is aseismic because of stable-sliding serpentinite hydrated by water from the underthrusting oceanic crust and sediments. For many subduction zones the downdip seismogenic width defined by these limits is much less than previously assumed. Within the narrowly defined seismic zone, most of the convergence may occur in earthquakes. Numerical thermal models have been employed to estimate temperatures on the subduction thrust planes of four continental subduction zones. For Cascadia and Southwest Japan where very young and hot plates are subducting, the downdip seismogenic limit on the subduction thrust is thermally controlled and is shallow. For Alaska and most of Chile, the forearc mantle is reached before the critical temperature, and mantle serpentinite provides the limit. In all four regions, the seismogenic zones so defined agree with estimates of the extent of great earthquake rupture, and with the downdip extent of the interseismic locked zone. 相似文献
13.
A. V. Klyuchevskii 《Journal of Volcanology and Seismology》2011,5(1):53-59
Correlation analysis techniques were used to study variations in the annual rates N of completely reported earthquakes with energy class K ≥ 8 that occurred from 1964 to 2001 in the Baikal Rift Zone (BRZ), in three subregions within that zone, and in six areas.
This correlation analysis of samples of annual rates of earthquakes N with different observation periods revealed two statistically significant episodes of short-lived synchronization between
the seismic processes in the BRZ, in the late 1960s and in the late 1970s to the early 1980s. The 1970–1980 episode stands
out because of its duration and the highest correlation level; this makes it the dominant phenomenon in the Baikal Rift seismicity
synchronization. The observed synchronization episodes between annual rates of earthquakes show that the seismic process was
activated at about the same time in different subregions of the BRZ, thus producing short-lived coherent increases in seismicity
rates. 相似文献
14.
A circum-earth shear zone at low-latitudes and episodic large earthquakes in it and the circum-Pacific seismic zone 总被引：1，自引：0，他引：1
MA Zongjin DU Pinren REN Jinwei & GAO Xianglin . Institute of Geology China Earthquake Administration Beijing China . Institute of Earthquake Science China Earthquake Administration Beijing China 《中国科学D辑(英文版)》2006,49(9):897-903
Although the temporal and spatial distribution of earthquakes looks like non-uniform, it is not com- pletely random. Locations of seismic zones are associ- ated with active tectonics. On a global or regional scale, several major or great earthquakes occur… 相似文献
15.
选用华北地震遥测台网和首都圈数字化地震遥测台网1993～2005年记录的2866个地震事件中的33487条P波和31822条S波的到时资料，计算得到了水平分辨率25km到50km之间的首都圈地区（385°N～41°N， 114°E～120°E）地壳三维P波和S波速度结构，并进一步获得泊松比分布.研究表明，首都圈地区P波和S波速度分布表现出强烈的横向不均匀性，浅层速度分布同地表地质结构分布相一致.分析得出震区强震多发生在低速体与高速体之间、低泊松比地区，且震源下部存在低速、高泊松比异常体.经过与其他地区研究结果相比较，对地震触发与流体的关系进行了探讨.流体在地震孕育及触发的过程中可能起着重要作用. 相似文献
16.
通过与更早地震资料的对比, 研究了鲜水河断裂带, 川滇地壳块体东带、 西带, 松潘、 龙门山断裂带以及整个川滇地区较长时间尺度的地震活动盛衰交替性。 结果表明, 川滇东带北段(鲜水河断裂带)、 松潘、 龙门山地震带及川滇西带中段和南段(主要是红河断裂带)的地震活动具有明显的几十到百年尺度的盛衰交替性。 而川滇东带中南段(安宁河-则木河-小江断裂带)与川滇西带北段(金沙江断裂带)在上述地震带的平静期里, 中强以上地震频次明显减少, 但有个别7级以上强震发生。 这样, 整个川滇地区地震活动的盛衰交替性呈现一种比较复杂的阶段性特征: 伴随频繁中强震的强震活跃期与突发强震活动期交替出现。 值得注意的是, 川滇地区从19世纪末开始的伴随频繁中强震的强震活跃期已超过百年, 目前出现长期平静, 应注意进入突发强震活动期的可能性。 根据川滇地区上一个突发强震活动期突发强震的空间分布, 推测未来的突发强震可能发生在南北向断裂带, 或其他方向断裂带与南北向断裂带的交汇部。 文中还对上述统计现象的机理作了简要讨论。 相似文献
17.
俯冲带作为地球最为庞大的循环系统的重要组成部分,已成为地球科学的研究热点之一.很多俯冲带,特别是环太平洋俯冲带内的中深源地震,在空间上呈明显的分层分布,并且各层地震具有不同的震源机制,即所谓的双地震带现象.本文简要介绍了环太平洋双地震带形态特征与震源机制的空间分布,并回顾了双地震带的几种成因模型.根据形态特征和震源机制的差异,中源深度的双地震带可以分为两类,其中,一类双地震带对应上、下二层分别为压缩和张性的地震分布;另一类双地震带的震源分布较浅,且其浅部地震以横向压缩为主.此外,日本本州东北俯冲带的地震分布可能是由三层地震带组成的,而且汤加、伊豆-小笠原地区还发现深源深度的双地震带.通过对双地震带的形态特征以及其热力学条件的研究,人们从抗弯作用、脱水脆化、相变断层等多方面,尝试建立解释双地震带成因的模型.目前,大多数研究利用数值计算结果,结合蛇纹石脱水脆化、相变断层模型,能够不同程度地分别解释中源和深源双地震带成因.不过,这些模型几乎相互独立,并不能同时解释中源和深源双地震带.有人试图尝试用统一模型解释中深源地震成因,例如,先前存在的断层模型,不过该模型还不很具有说服力.也可能是多种因素的联合作用,共同影响着俯冲板内的温度场、应力场分布. 相似文献
18.
The better located earthquakes from the Earthquake Data File of NOAA during the period from 1967 to December 1971 define a seismic zone dipping eastward below Chile with a thickness of 20–70 km. Vertical sections were used to examine the morphology of the zone. The orientation of the vertical sections and the limits of the area projected onto the sections were chosen to produce plots of the seismic zone showing the least thickness and steepest dip. These conditions should be characteristic of sections which are perpendicular to the seismic zone. Seven segments that differ in strike and dip were found. The segments range in dip from 20° to 30° and have lengths of 300–850 km. There are offsets of the seismic zone between adjacent segments of up to 50 km and changes in strike of up to 30°. There are similar offsets in the historically active volcanic chain. The breaks in the deep seismic zone correspond to abrupt changes in topography and tectonic structures. The margins of great earthquake aftershock zones correspond well with the segment boundaries proposed here. 相似文献
19.
地震破裂区是地震时沿发震断裂带的同震错动面或破裂面在地表的垂直投影区域,指示了震源断层/破裂的位置与尺度。确定过去长期的强震/大地震破裂区是鉴别地震空区、研究与预测强震危险性的重要基础。对于现代强震,破裂区可运用多种现代技术方法确定,但对于历史强震,破裂区确定的方法需要探索与发展。以华北地区为例,研究利用烈度/等震线资料、结合地震构造与震区地表地质环境等信息确定历史强震破裂区的方法,并开展应用试验。结果表明:研究区现代地震破裂区延伸的烈度区间与极震区烈度、震区环境之间存在密切关系,基于这种关系建立了2条经验准则,可分别用于根据烈度分布确定华北2类震区环境(基岩区和厚层第四纪松散堆积覆盖区)历史强震破裂区的位置与延伸。文中还提出通过综合地震构造、现代小震/余震分布等信息,辅助确定历史强震破裂区横向宽度的思路与途径。作为应用试验,文中确定了5次历史地震的破裂区,结果表明本文发展的经验准则及相应方法适用于华北地区历史强震破裂区的确定。 相似文献