共查询到16条相似文献，搜索用时 359 毫秒
1.
前震研究进展综述 总被引：1，自引：0，他引：1
简要介绍了当前国内外前震研究领域的一些进展。对比了不同前震定义条件下前震序列的共性特征,对几种主要的前震机理及主要的前震识别方法进行了简要综述,对其特点及存在的问题进行了评述和讨论。前震指主震之前在主震断层面上、紧邻主震破裂起始点发生的小地震。主震发生之前的一系列前震活动构成前震序列。在不同的前震定义条件下,具有“直接前震”的震例比例从10%至40%不等。理论上前震可用级联应力触发或预滑动模型进行解释。前震空间上主要集中分布在距离主震10~75km范围内,但其时间分布形式非常复杂,大多发生在主震前1~2天,部分前震序列的地震活动率显示明显的加速特征,但许多前震序列单独来看却往往显示主-余型序列的衰减特征。序列地震震源机制一致、序列b值偏低是前震序列最突出的特征。前震的发生与主震破裂形式和构造环境似有一定关系,在有限的前震震例中,逆冲型主震似乎具有相对更多的前震。部分震例的研究结果显示,随主震的临近,前震震源深度有逐渐下迁的特点。到目前为止,震前很难判定一次地震或一个地震序列是否前震或前震序列,所使用的前震识别主要有基于统计类比的方法、基于震源机制一致及衍生的相关方法以及基于对地震成核过程精细检测的方法。从现有不多的震例研究结果来看,尽管地震时空丛集和震源机制高度一致是前震序列的最显著特征,但却不是判定前震序列的充分条件。由于成核的破裂扩展速度和滑动位移有随时间较快增大的趋势,因而基于对地震成核过程精细检测的方法有望在前震识别中发挥更为重要的作用,但需更多震例进行验证。 相似文献
2.
介绍了当前国内外前震研究领域的一些进展。 对比了不同前震定义条件下前震序列的共性特征, 对几种主要的前震机理及主要的前震识别方法进行了简要综述, 对其特点及存在的问题进行了评述和讨论。 前震指主震之前在主震断层面上、 紧邻主震破裂起始点发生的小地震。 主震发生之前的一系列前震活动构成前震序列。 在不同的前震定义条件下, 具有“直接前震”的震例比例从10%至40%不等。 理论上前震可用级联应力触发或预滑动模型进行解释。 前震空间上主要集中分布在距离主震10~75 km范围内, 但其时间分布形式复杂, 大多发生在主震前1~2天, 部分前震序列的地震活动率显示明显的加速特征, 但许多前震序列单独来看却往往显示主-余型序列的衰减特征。 序列地震震源机制一致、 序列b值偏低是前震序列最突出的特征。 前震的发生与主震破裂形式和构造环境似有一定关系, 在有限的前震震例中, 逆冲型主震似乎具有相对较多的前震。 部分震例的研究结果显示, 随主震的临近, 前震震源深度有逐渐下迁的特点。 到目前为止, 震前很难判定一次地震或一个地震序列是否为前震或前震序列, 所使用的前震识别主要有基于统计类比的方法、 基于震源机制一致及衍生的相关方法以及基于对地震成核过程精细检测的方法。 从现有不多的震例研究结果来看, 尽管地震时空丛集和震源机制高度一致是前震序列的最显著特征, 但却不是判定前震序列的充分条件。 由于成核的破裂扩展速度和滑动位移有随时间较快增大的趋势, 因而基于对地震成核过程精细检测的方法有望在前震识别中发挥更为重要的作用, 但需更多震例进行验证。 相似文献
3.
4.
5.
6.
论述了由数字化地震记录测定震级谱,频谱的特征方法,将天文学上对天体星等色指数的办法移植到地震学中,用模拟地震记录测算４种震级标度所定义的震级,进而计算“震级色指数”,并用以判别地震系列的类型;１）红地震;２）蓝地震;３）前震型;４）混合震群型;５）单主余震型;６）孤立型地震的频谱生物及其频谱成分标志。 相似文献
7.
2021年5月21日漾濞发生MS 6.4地震,震前地震活动异常明显,中长期阶段云南地区3级地震活动水平较低,滇西北地区出现长达456天的4级地震平静;短临阶段震中区附近出现3—4级地震条带;临震阶段中小地震活动由外围地区开始向震中区迁移,震中区出现直接前震。 相似文献
8.
前震或广义前震识别的频谱偏移法及其应用研究 总被引：3，自引：0，他引：3
在前期研究的基础上,本文提出了一种前震或广义前震识别的频谱偏移法。其判定指标为,正常背景的中等震级地震事件频谱较宽,而具有前震或广义前震性质的中等震级地震具有频带变窄且向低频端偏移集中的特征。究其根源可能与强震前震源区或主震相关区域亚稳态扩展破裂或区域介质破碎损伤、裂隙扩展成核等过程有关。对2010年4月14日青海玉树7.1级、2014年2月12日新疆于田7.3级等地震前震的计算结果显示,2次前震的频谱都发生了偏移,且与非前震性同等震级地震频谱差异明显。 相似文献
9.
建造了一个前震和前震序列发生的模型，前震与主震的发生假定是由于原有裂隙的突然并合所致。如果裂隙端点应力强度因子超过某一临界值则并合发生。在亚临界状态，每一裂隙由于应力腐蚀经历准静态的加速扩展，直到达到临界状态，最终发育成灾变。前震发生的比率随着主震临近而增加，可用一个时间的幂函数描述。幂法则中的指数与裂隙大小、间隔和破裂强度的分布无关。这种普遍性意味着前震图象对于预报大震发生的时间将是有用的识别。然而，我们发现在能量释放的图象中存在值得考虑的差异。如果人们具有描述障碍体强度和几何形态的“先验”信息，就有希望根据前震序列事件的震级预报大地震的震级。 相似文献
10.
11.
Using the match-and-locate method to characterize foreshocks of the July 2019 MW6.4 Ridgecrest,California earthquake 
下载免费PDF全文
下载免费PDF全文 The July 2019 MW6.4 Ridgecrest, California earthquake and its distinct foreshocks were well recorded by local and regional stations, providing a great opportunity to characterize its foreshocks and investigate the nucleation mechanisms of the mainshock. In this study, we utilized the match-and-locate (M&L) method to build a high-precision foreshock catalog for this MW6.4 earthquake. Compared with the sequential location methods (matched-filter + cross-correlation-based hypoDD), our new catalog contains more events with higher location accuracy. The MW6.4 mainshock was preceded by 40 foreshocks within ～2 h (on July 4, 2019 from 15:35:29 to 17:32:52, UTC). Their spatiotemporal distribution revealed a complex seismogenic structure consisting of multiple fault strands, which were connected as a throughgoing fault by later foreshocks and eventually accommodated the 2019 MW6.4 mainshock. To better understand the nucleation mechanism, we determined the rupture dimension of the largest ML4.0 foreshock by calculating its initial rupture and centroid points using the M&L method. By estimating Coulomb stress change we suggested that the majority of foreshocks following the ML4.0 event and MW6.4 mainshock occurred within regions of increasing Coulomb stress, indicating that they were triggered by stress transfer. The nucleation process before the ML4.0 event remains unclear due to the insufficient sampling rate of waveforms and small magnitude of events. Thus, our study demonstrates that the M&L method has superior detection and location ability, showing potential for studies that require high-precision location (e.g., earthquake nucleation). 相似文献
12.
James H. Dieterich 《Pure and Applied Geophysics》1988,126(2-4):589-617
Current methods for calculation of long-term probabilities for the recurrence of large earthquakes on specific fault segments are based upon models of the faulting process that implicitly assume constant stress rates during the interval separating earthquakes and instantaneous failure at a critical stress threshold. However, observations indicate that the process of stress recovery following an earthquake involves rate variations at all time scales in addition to stress steps caused by nearby earthquakes. Additionally, the existence of foreshocks, aftershocks and possible precursory processes suggest that there may be significant time dependence of the earthquake nucleation process. A method for determining the conditional probabilities for earthquake occurrence under conditions of irregular stressing is developed that could be useful at all time scales including those pertinent to short-and intermediate-term prediction. Used with models for earthquake occurrence at a stress threshold, the addition of variable stressing introduces a simple scaling of the conditional probabilities by stress level and stress rate. A model for the time-dependent nucleation of earthquake slip has been proposed recently that is based upon laboratory observations of fault strength. This failure criterion results in large but relatively short duration changes in the probability of earthquake recurrence particularly following stress steps. Applied to populations of earthquakes the models predicts a 1/t decay of seismicity following stress steps as observed for aftershocks and for frequency of foreshock-mainshock pairs. The model suggests that variations of seismicity rates of small earthquakes in the nucleation zone of the expected earthquake directly indicate variations in probability of recurrence of the large earthquake. 相似文献
13.
David J. Varnes 《Pure and Applied Geophysics》1989,130(4):661-686
During 11 sequences of earthquakes that in retrospect can be classed as foreshocks, the accelerating rate at which seismic moment is released follows, at least in part, a simple equation. This equation (1) is
,where
is the cumulative sum until time,t, of the square roots of seismic moments of individual foreshocks computed from reported magnitudes;C andn are constants; andt
fis a limiting time at which the rate of seismic moment accumulation becomes infinite. The possible time of a major foreshock or main shock,t
f,is found by the best fit of equation (1), or its integral, to step-like plots of
versus time using successive estimates oft
fin linearized regressions until the maximum coefficient of determination,r
2,is obtained. Analyzed examples include sequences preceding earthquakes at Cremasta, Greece, 2/5/66; Haicheng, China 2/4/75; Oaxaca, Mexico, 11/29/78; Petatlan, Mexico, 3/14/79; and Central Chile, 3/3/85. In 29 estimates of main-shock time, made as the sequences developed, the errors in 20 were less than one-half and in 9 less than one tenth the time remaining between the time of the last data used and the main shock. Some precursory sequences, or parts of them, yield no solution. Two sequences appear to include in their first parts the aftershocks of a previous event; plots using the integral of equation (1) show that the sequences are easily separable into aftershock and foreshock segments. Synthetic seismic sequences of shocks at equal time intervals were constructed to follow equation (1), using four values ofn. In each series the resulting distributions of magnitudes closely follow the linear Gutenberg-Richter relation logN=a–bM, and the productn timesb for each series is the same constant. In various forms and for decades, equation (1) has been used successfully to predict failure times of stressed metals and ceramics, landslides in soil and rock slopes, and volcanic eruptions. Results of more recent experiments and theoretical studies on crack propagation, fault mechanics, and acoustic emission can be closely reproduced by equation (1). Rate-process theory and continuum damage mechanics offer leads toward understanding the physical processes. 相似文献
14.
In order to examine the relationship between anomalous crustal deformations and subsequent large earthquakes, we compiled and examined data on preseismic anomalous crustal deformations for two earthquakes that occurred in and around the Japanese Islands in recent years. We found that the slip on a downward extension of a seismogenic fault accelerates before the main shock and that the average slip velocity is inversely proportional to the time remaining until the main shock occurs. 相似文献
15.
We study the October 18, M
W = 7.1, 1992 Atrato earthquake, and its foreshocks and aftershocks, which occurred in the Atrato valley, northwestern Colombia. The main shock was preceded by several foreshocksof which the M
W = 6.6, October 17 earthquacke was the largest. Inparticular, we examine foreshocks and aftershocks performing joint-hypocenter relocations using high quality Pn and Sn wave readingsfrom permanent regional networks. We observed a few hours prior to the main shock a sudden increase of foreshocks. Maybe this could be used as a predictor since foreshocks have been known for other major events in the region. Our locations align for 90 km with a trend of 5° ±4° in agreement with the Harvard CMT solution showing the faultplane trending 9° to be the plane of rupture. In relation to theepicenter of the main shock, maximum intensities were located to thesouth, consistent with a rupture that traveled from north to south witha larger energy release in the south as suggested by an empirical Green'sfunction study (Li and Toksöz, 1993; Ammon et al., 1994). The boundarybetween the Panama and North Andes blocks has been placed close to thePanama-Colombia border as either a sharp boundary or a diffuse zone. TheAtrato earthquake, however, shows that the plate boundary between thePanama and North Andes microblocks is a diffuse deformation zone. Thiszone has a width of at least 2° stretching from 78°W to 76°W. Quantification of earthquake moment release (during the past30 years) in this zone shows a similar amount of moment release in thewestern and eastern parts of this zone. 相似文献