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1.
景谷6.6级、鲁甸6.5级地震序列应力降变化对比研究 总被引：1，自引：1，他引：0
利用云南2014年10月7日景谷6.6级、8月3日鲁甸6.5级地震序列的波形与震相资料,消除区域地震波衰减与台站场地响应后,计算得到2次地震序列的应力降。结果显示,在研究所涉及的震级范围内,应力降呈现随震级增大而增大的趋势。为尽可能消除震级对应力降的影响,对比了相同震级档地震的应力降,结果显示,景谷地震序列的平均应力降明显高于鲁甸地震,这可能与2次6.5级左右地震后震源区的应力状态有关。从序列余震应力降的时、空变化对比来看,景谷6.6级地震后至2014年12月6日5.8、5.9级强余震发生前,应力降变化呈现先缓慢下降、进而转折升高并持续高值的变化过程;同时,高应力降地震在空间上主要集中于5.8级强余震区域。这表明,主震发生后经过一个较短期的调整之后,5.8级强余震震源区的应力环境可能持续增强。5.8、5.9级强余震发生后,地震序列应力降快速下降至相对稳定状态。研究表明,2次6级左右强余震发生后,震源附近区域应力得到一定程度的释放,应力环境降低,地震序列活动也趋于结束。对于后续没有强余震发生的鲁甸地震序列,余震应力降小于景谷地震序列相同震级档地震的平均应力降,同时,主震后余震序列的应力降在时间上几乎未发生太大的变化;结合主震能量释放特点推测,震源区的应力在主震破裂过程中已得到较多的释放,主震后震源区应力变化呈现逐渐恢复的过程,这可能是鲁甸地震余震活动明显较弱,后续亦未有较强余震发生的原因之一。 相似文献
2.
在1966年发生6.8和7.2级邢台地震的余震区里,从1976年1月至1985年11月已记录到约6000次地震,其中最大的两次地震是1981年11月9日M_L=5.8和1985年11月30日M_L=5.6的地震。本文利用P波初动半周期,测定了这一时间段里发生的69次M_L=2.7—4.4的地震的震源参数。应力降在0.01兆帕到10兆帕的范围内变化,且主要集中在0.1兆帕和1兆帕之间,因此取1兆帕以上为高应力降,用以评定该区的应力积累情况。震源半径的变化范围大,但在M_L≤3.7的范围内不随M_L而变大,而应力降则随M_L而增大。1981年的5.8级地震和1985年的5.6级地震,虽然在震前、震后的地震活动上都完全不一样,但其共同点是:震前出现的高应力降地震比较多,且其应力降的数值有随时间增高的趋势。 相似文献
3.
4.
本文利用四川省区域固定地震台网观测记录到的2008年汶川8.0级地震序列的资料,从中挑选部分台站和地震资料,在精确扣除了余震区地震波衰减与台站场地响应后,计算得到了汶川地震序列中1070次ML≥3.0级地震的震源参数,结果显示,地震矩与震级之间有较好的线性关系,应力降和视应力的大小与震级大小有关.利用ML3.0级地震资料得到的应力降的时空演变过程研究结果表明,汶川余震序列地震应力降总体上随时间是一个衰减过程,预示着主震发生后整个余震区应力降呈逐渐衰减的状态.主震发生之后,以虎牙—北川—安县为界,空间上龙门山断裂带上地震活动水平和应力降具有明显的分段性.5月17日之前ML≥5.0余震主要集中在龙门山断裂带北川以西,由于地震释放了较多应力,该地区应力降较低,而北川至青川之间地震活动水平相对较弱,应力降一直处于高值水平.5月17日之后,ML5.0余震活动主体地区则转移到北川至青川之间,在该段发生了5月25日青川6.4级最大余震,在这之后,整个余震序列应力降随时间变化开始趋于平稳. 相似文献
5.
地震应力降标志震源破裂过程中作用在断层系统上的应力释放水平,是刻画震源物理过程和预测震源辐射特性的重要参数.地震应力降主要受控于构造环境、震源机制和地震类型等.观测得到的应力降还受到观测频带的影响,所以它的绝对值难以准确测定.采用体波、面波以及零频观测（大地测量、GPS、InSAR）等不同类型的数据获得的应力降也存在差异.对于地震波数据,通常采用间接方法去除传播路径中的衰减效应并获得震源激发谱,进而估计应力降.随着宽频带地壳Lg波衰减模型的建立,可以构建直接校正路径衰减的方法,从而获得对Lg波震源激发函数的准确估计.进而通过对观测和理论震源谱的拟合获得整个地震序列中各个地震的标量地震矩、拐角频率和高频下降率等震源参数,再根据断层模型计算应力降.本文分别以青藏高原东缘典型的构造地震2017年Ms7.0九寨沟地震和潜在的工业注水诱发地震2019年Ms6.0长宁地震为例,计算两个地震序列应力降的时-空变化过程,探索构造地震与诱发地震之间的潜在的物理差异. 2017年九寨沟地震的主震应力降为27 MPa,余震震级和应力降均呈快速下降趋势. 2019年长宁地震的主震应力降为32 MPa,余震序列... 相似文献
6.
2001年永胜6.0级地震的余震序列应力降研究 总被引：5，自引：2，他引：3
根据Haskell提出的一个统计不均匀随机震源ω -立方模型 ,导出了用震源参数估算地面运动峰值速度的量度 ,从而建立了地面运动峰值速度 (r·v)直接与震源参数的依赖关系 ,即 ,以地震矩、应力降作为标度律参数 ,预测的地面峰值速度按照M01 2 Δσ1 2 标度。对永胜地震近场数字地震记录的峰值速度参数资料的分析表明 ,这样的标度关系更适合对小地震的震源参数估算的统计研究。假定Q因子随频率线性变化的指数衰减项作为地震波传播距离的非弹性衰减 ,导出用地面运动峰值速度直接估算地震应力降Δσ的关系 :lg (r·v e-qr) =- 6 0 +0 5lgM0 +0 5lgΔσ ,测定了 2 0 0 1年永胜M6 0级地震近场数字地震台网观测的 1 0 0多次余震序列的地震应力降。结果给出 ,震级在 0 5 相似文献
7.
采用新疆区域台网记录的2012年6月30日新源、和静交界M_L6.8地震序列的数字波形资料,研究分析了余震序列应力降的变化特征及其地震序列震源机制的相关性。采用波谱分析方法和Brune震源模型,计算了新源、和静交界M_L6.8地震序列震源参数、地震序列中不同事件在相同台站的体波零频震源谱值、地震谱振幅相关系数;并对地震序列震源机制解进行聚类分组。结果表明:①在余震序列平静阶段,应力降呈平稳态势,强余震前应力降出现升高-回落变化过程;②滑动平均谱振幅相关系数在主震后发散,表明余震的震源机制解与主震的相关性降低;③震源机制解聚类分组结果显示,M_L6.8地震序列主要以走滑型地震为主,主压应力轴呈近NS向,与近NS向的构造应力场结果基本一致,一定程度上显示了地震前天山中段受NS向水平挤压应力作用明显;④震级、震源机制演化表明,强余震前震源机制解表现较好的一致性,显示了区域应力场控制作用增强,对后续强余震发生具有预测意义。 相似文献
8.
青岛崂山ML 4．1地震序列应力降变化研究 总被引：1，自引：1，他引：0
根据Andrews谱积分方法,采用近震源Brune圆盘模型,研究了2003年6月3日青岛崂山ML4.1地震序列破裂过程中应力降变化情况.结果表明,崂山序列主震静应力降为24 MPa,动态应力降大约为静态应力降的2.2倍;崂山序列余震应力降普遍低于5 MPa,约有80%的余震应力降小于1 MPa,显示出与主震断层面有关的余震低应力降现象,这说明主震的破裂与余震破裂过程之间存在明显的差别.这种现象与崂山序列的弱强度衰减一致,表明此次序列的余震属于低能量破裂过程.计算结果显示:①由Andrews谱积分方法得到的小震应力降与震级大小存在一定的相关性;②小应力降事件的静态应力降和动态应力降的比值普遍小于1,未发现明显的应力降之比与Brune应力降之间的关系. 相似文献
9.
利用谱分析方法对河北省测震台网2016年1月—2020年7月唐山老震区(117.5°～119.5°E,39°～41°N)85次M_L≥2.5地震进行震源参数分析,发现该时段唐山老震区应力降范围在0.1～10.3MPa,主要集中在0.1～1.0MPa,其中应力降小于2MPa的地震占81%。当2.5≤M_L≤3.5时,应力降、拐角频率与震级之间无明显的对应关系;ML≥4.0地震较少,但应力降有随震级增大而增大的趋势,拐角频率有随震级增大而减小的趋势。2019年12月5日河北丰南M4.5地震和2020年7月12日唐山M5.1地震之间发生了 7次M_L≥2.5地震,震级范围为2.5≤M_L≤2.8,提取该震级范围的震源参数进行时空分析,发现唐山M5.1地震前有2次明显的高应力降事件,2次高应力降事件呈现出应力降数值高、拐角频率高、震源尺度小的特点,表明单位体积所释放能量较多。2次高应力降事件均发生在唐山M5.1地震震中17km范围内,可能是唐山M5.1地震前震源区构造应力较高的一个标志。 相似文献
10.
基于云南数字地震台网记录的2008年盈江地震序列的数字波形资料,采用波谱分析方法和Brune震源模型,得到盈江地震序列的震源参数。利用两次地震事件的相同台站的震源谱参数（零频振幅）计算谱振幅相关系数,据此对地震的震源机制进行聚类分组,并收集和对比地震序列已知的震源机制解结果,发现每组内震源机制解P轴的相关性较好,且相关系数越大,P轴的方位角就越接近。将盈江地区划分为三个研究区,联合震源参数的应力降和聚类分组中每组的平均震源机制解结果研究地震序列发生过程中应力的释放水平和应力场方向变化特征。结果表明：不同阶段震源机制解类型的变化和转化特征一定程度上反映了孕震过程中区域应力场随时间的变化特征,并且地震震源机制解类型在时间段上的集中并向区域构造应力场方向转换的现象可能是发生强震的标志。震源机制解分组类型和对应类型的地震的应力降有一定依赖关系,震源机制解类型反映的应力场与区域应力场接近的地震应力降高,震源机制解类型反映的应力场与区域应力场差距较大的地震应力降普遍较低。 相似文献
11.
ＥｓｔｉｍａｔｉｏｎｏｆｓｅｉｓｍｉｃｓｔｒｅｓｄｒｏｐｆｒｏｍｔｈｅｐｅａｋｖｅｌｏｃｉｔｙｏｆｇｒｏｕｎｄｍｏｔｉｏｎＪＩＡＺＨＥＮＧＱＩＮ（秦嘉政）ＺＵＹＩＮＬＩＵ（刘祖荫）ＸＩＡＯＤＯＮＧＱＩＡＮ（钱晓东）ＱＩＮＧＹＩＮＸＩＥ（谢庆... 相似文献
12.
Apparent stress and stress drop for intraplate earthquakes and tectonic stress in the plates 总被引：1，自引：0，他引：1
The magnitude of shear stress in the lithosphere is bounded from below by the apparent stress and stress drop during intraplate earthquakes. Apparent stresses and stress drops for a number of mid-plate earthquakes are calculated from the earthquake magnitude, SH wave amplitude spectra, and estimates of the length of the fault zone. Apparent stresses vary between 0.1 and 2 bars, ifm
b
is used as a measure of seismic energy, and stress drops lie between 2 and 70 bars. There is no systematic difference in either apparent stress or stress drop between these intraplate events and typical plate boundary earthquakes. These bounds on intraplate shear stresses are consistent with the inference from current models of plate tectonic driving forces that regional stress differences in the plates are typically on the order of 100 bars. The highest stress drops measured for midplate earthquakes under this model represent nearly total release of local tectonic stress. 相似文献
13.
使用谱比法计算得到四川长宁地区2018年12月至2019年7月期间442个地震的震源参数,并进一步分析了震源参数之间的相互关系及应力降的时空分布特征。研究区的地震活动主要集中在长宁背斜核部和南部建武向斜页岩气开采区。研究结果显示,该地区ML1.3~4.7地震的应力降位于0.02~7.26MPa范围内,超过90%的地震应力降小于2MPa,应力降总体呈现随震级增大而增大的趋势,但与震源深度的关系并不明显。长宁MS6.0地震发生之前,震源区地震的应力降总体处于较低水平,主震发生之后,短期内余震的应力降较高,随后快速衰减。这些高应力降地震空间上主要集中在长宁余震区的西北段,也是余震强度较大、发生了几次MS>5.0强余震的位置。建武向斜页岩气开采区地震的应力降总体略低于长宁背斜地区,但差异并不显著。 相似文献
14.
The earthquake stress-drop values of two sequences were accurately calculated after taking away the effects due to regional earthquake anelastic attenuation and station site response, using waveform data and seismic phase data of sequences of the Jinggu MS6.6, and Ludian MS6.5 earthquakes in Yunnan. These results show that the stress drop with magnitude increases within the scope of this study of magnitude. After eliminating the influence of the magnitude, the average value of stress-drop in the Jinggu sequence is higher than that of the Ludian sequence at the same magnitude range. This may be related to the stress state in different regions. In terms of the changes of time and space of stress-drop, before MS5.8 strong aftershock, the stress-drop is "slowing down-turning up-keeping a high value" after the mainshock, meanwhile, almost all of the abnormally high stress drop value is distributed around the MS5.8 strong aftershock, showing that the stress environment in the region was increasing after the mainshock. And after the MS5.9 strong aftershock, stress-drop rapidly declines to a relatively stable state, meanwhile, the high value of stress-drop is distributed around the strong aftershock, showing that the regional tectonic stress gets more fully release, its stress environment begins to rapidly decrease. For the Ludian sequence without a strong aftershock occurring, the average value of stress drop is lower than that of the Jinggu earthquake sequence at the same magnitude range, while at the same time, the stress-drop of the aftershock sequence almost hasn''t changed much. In the time after the mainshock, combined with the release characteristics of the main energy, the stress in the region is excessively released, the subsequent stress in the region gradually returns to normal. This may be the reason why the activity of Ludian aftershocks significantly was weaker and subsequently there were no strong aftershocks occurred. 相似文献
15.
利用山东台网记录的长岛震群2017年2月14日—9月1日期间的波形与震相资料研究长岛地区非弹性衰减系数,得到该地区介质平均Q值与频率f的关系式为Q(f)=363.9f1.374 1。采用Moya等[1]提出的利用遗传算法联合反演得到长岛周边台站的场地响应,根据Brune模型震源参数计算公式求解长岛震群序列地震震源参数。结果显示,各个震源参数之间均存在一定的相关关系,地震矩随ML震级的增大而增加,地震矩与破裂半径R之间存在半对数关系,拐角频率fc随地震矩的增大而减少;长岛地震序列的应力降数值普遍偏小,最大不超过0.9MPa,这意味着长岛震源区整体构造应力较低,也可能指示长岛震群为低摩擦应力的断层作用;震源参数随时间的变化方面,整体而言,长岛震群地震应力降变化起伏很大,在M4.1地震发生前,拐角频率与应力降均发生快速下降后随即翻转上升的现象,证明在M4.1地震发生前震源区整体应力的挤压逐渐增强。 相似文献
16.
The source parameters for 213 Bhuj aftershocks of moment magnitude varying from 2.16 to 5.74 have been estimated using the
spectral analysis of the SH- waveform on the transverse component of the three-componnet digital seismograms as well as accelerograms.
The estimated stress drop values for Bhuj aftershocks show more scatter (Mo0.5 to 1 ∞ Δσ) toward the larger seismic moment values (log Mo ≥ 1014.5 N-m, larger aftershocks), whereas, they show a more systematic nature (Mo3 ∞ Δσ) for smaller seismic moment (log Mo < 1014.5 N-m, smaller aftershocks) values. This size dependency of stress drop has also been seen from the relation between our estimated
seismic moment and source radius, however, this size-dependent stress drop is not observed for the source parameter estimates
for the other stable continental region earthquakes in India and around the world. The estimated seismic moment (Mo), source
radius (r) and stress drop (Δσ) for aftershocks of moment magnitude 2.16 to 5.74 range from 1.95 × 1012 to 4.5 × 1017 N-m, 239 to 2835 m and 0.63 to 20.7 MPa, respectively. The near-surface attenuation factor (k) is found to be large of the
order of 0.03 for the Kachchh region, suggesting thick low velocity sediments beneath the region. The estimated stress drop
values show an increasing trend with the depth indicating the base of seismogenic layer (as characterized by larger stress
drop values (>15 MPa)) lying in 22–26km depth range beneath the region. We suggest that the concentration of large stress
drop values at 10–36km depth may be related to the large stress/strain associvated with a brittle, competent intrusive body
of mafic nature. 相似文献
17.
According to the rupture dynamics of earthquakes, variations of the apparent stress and the difference between the static
stress drop and the dynamic stress drop during the rupture of earthquakes are analyzed for the July 20, 1995 M
L=4.1 Shacheng, Hebei, China, earthquake sequence. Results obtained show that the apparent stress for main-shock is about 5
MPa, and the average apparent stress for aftershocks 0.047 MPa. During the rupture of the main-shock, the dynamic stress drop
is approximately 1.6 times greater than the static stress drop with the difference of nearly 2.7 MPa. The dynamic stress drop
is less than the static stress drop for all aftershocks with the average difference of −0.75 MPa. Therefore, when the mainshock
occurs the final stress on the focal fault is higher than the dynamic frictional stress, corresponding to that the fault is
abruptly locked. When the aftershocks occur the final stress on the focal fault is lower than the dynamic frictional stress,
corresponding to that the fault overshoots. It can be seen from the above results that there could be some differences in
the physic processes between the mainshock and the aftershocks.
Contribution No. 05FE3013, Institute of Geophysics, China Earthquake Administration. 相似文献
18.
The data analysis of the source parameters of five sets of earthquake sequences, aftershocks and earthquakes scattered in
a region shows that the scalar seismic moment is correlated with the linear size of the fault and the static stress drop.
We tentatively imply that a correlation also exists between the radius of the faults and the static stress drops and it is
suggested that the static stress drop may be decreasing with increasing radius of the source. It is shown that the density
distribution of the source radius, calculated through the source rupture duration obtained from the body wave pulse (Boatwright,
1980) using the time T between the P-wave onset and the first zero crossing on the seismogram, may be represented by a power law as the density
distribution of the stress drops and of the moment which are also computed. It is also suggested, and tentatively verified,
that the density distribution of the areas of the broken barriers on the faults is similar to that of the density distribution
of the static stress drops. It is finally suggested that the seismicity of a region may be studied two-dimensionally as a
function of the stress drop and the radius of the source instead of the classic b and b0 values. Concerning the discussion on the range of the values of the static stress drop, whether it is almost constant in
a seismic region and varies only from one region to another, it is seen that in the aftershocks of the 1994 Northridge earthquake
it covers a range of almost 5 orders of magnitudes. Finally it is ascertained that the density distribution of the source
parameters does not give equipartition of seismic moment release. 相似文献
19.
Characteristics of recent tectonic stress field in Jiashi, Xinjiang and adjacent regions 总被引：1，自引：0，他引：1
崔效锋 《地震学报(英文版)》2006,19(4):370-379
Introduction The Pamirs region where Jiashi is located is one of the most active regions of continental plate dynamics in China. Frequent earthquakes here, especially several strong earthquakes oc- curred in 1997 and 2003, have provided excellent conditions for studying the tectonic stress field in this region and a large number of results (GAO and WEN, 2000; GAO et al, 2004; XU, 2001; ZHOU et al, 2001) have been obtained. Although different methods and data were used, under- standings … 相似文献
20.
Based on the digital waveform data recorded by Xinjiang Digital Seismic Network for the Xinyuan-Hejing M_L6.8 earthquake sequences of June 30,2012,this paper analyzes the stress drops of earthquake sequences and the correlation coefficients of focal mechanisms significant for strong aftershocks.Firstly,the source parameters of the Xinyuan-Hejing M_L6.8 earthquake sequences are obtained by applying the spectrum analysis and the Brunes source model.Then,the correlation coefficients of spectral amplitudes are calculated using the low-frequency spectral amplitude recorded by the same station for the different events.Finally,based on the results of the correlation coefficients of spectral amplitudes,the events with similar focal mechanisms are grouped using the clustering method.The results show that:(1)The stress drop values show a steady trend in the aftershock sequence calm period and the stress drop values show a rise-fall in strong aftershocks.(2)The moving average correlation coefficient of amplitude spectrum begins to spread after the main shock.It shows that the correlation decreases between the main shock and the aftershocks in mechanisms.(3)The results of focal mechanism groups show that the earthquake sequences are mainly strike slips.The stress distribution of the main pressure axis is nearly NS,which is the same as the structural stress field.(4)The magnitude and mechanism show that there is an agreement before the strong aftershock,which shows that the regional stress field is enhanced. 相似文献