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1.
高原  吴忠良 《中国地震》1995,11(2):147-160
远震体波宽频带记录可以用来研究震源参数和破裂过程,利用宽频带地震记录的P波振幅,可以找到一种较方便地得到一次中强地震的震源机制解的计算方法。1993年10月2日中国新疆南部Mb6.2地震是一个较为复杂的事件,利用宽频带波形资料和本文提出的一种简化的计算震源两个子事件相对位置的方法分析后认为,这次事件实质上是两次破裂的结果。Mb6.2地震事件发生前约2.3秒,有另一个小地震事件发生,两个事件之间的相  相似文献   

2.
本文用CDSN宽频带数字记录,计算了不对称双侧破裂模式的P波远场位移谱,用频谱方法研究中强地震的震源参数,并将它应用于1989年9月22日四川小金MS=6.6级地震的震源参数研究中。研究结果表明,断层长度为8.4km;宽度为2.9km;动力学参数:地震矩为4.7×1017N·m;平均位错64.6cm;应力降18.9×105Pa.并用余震震源深度分布的空间图象证明了:地震断层为走向NW33°的走滑断层,断层面倾向为北东,倾角约为20°。  相似文献   

3.
鄞县ML3.9和ML4.7地震的震源参数   总被引:3,自引:0,他引:3  
1993年2月26日和1994年9月7日在浙江宁波鄞县发生了ML3.0和ML4.7地震。本文使用华东地区部分台站的地震记录资料给出了这两次地震的震源机制和震源参数。其主要结果是:该区的主压应力方向约为北东60°;3.0级地震的破裂方向为SSW,破裂速度为2.7km/s,破裂尺度为0.39km;4.7级地震的破裂方向为NWW,破裂速度为2.3km/s,破裂尺度为0.41km。  相似文献   

4.
提出了一种以小震的记录作为格林函数来成像中强地震破裂增长的反演方法。该方法通过迭代法中同时拟合多台的P、S波形,估计了子事件相对格林函数事件的破裂时间和振幅。我们用小事件作为格林函数反演了发生在帕克菲尔德地区的2次中强地震的加速度图。第1次地震(M=4.6)于1993年11月14日发生在米德尔山,震源深度11km,在下一次帕克菲尔德主震的假定孕震区内。第2次地震(M=4.7)于1994年12月20  相似文献   

5.
2006年12月26日12点26分27秒(GMT)台湾南部滨海发生M_s7.2(Harvard CMT)级地震.震中位于台湾南部滨海之南海次板块与菲律宾海板块碰撞引发造山作用生成的海洋增生楔内,这次地震是该区域百年来震级最大的地震.我们利用中国数字地震台网(CSDN)和美国地震学联合研究所(IRIS)提供的上地幔及远场范围宽频带P波垂向记录资料,基于点源和有限断层模型进行波形拟合反演,获得这次地震的震源机制解并给出了震源破裂过程.反演结果表明,本次地震为东倾正断层兼小幅度走滑破裂事件,断层面走向为341.5°,倾角为77.9°,震源深度6 km.所得正断层震源机制解表明,地震可能与板块的拆离(break-off)作用引发的在台湾造山带局部存在伸张作用力有关.  相似文献   

6.
郭志  高星  王卫民 《地球物理学报》2008,51(4):1103-1113
2006年12月26日12点26分27秒(GMT)台湾南部滨海发生Ms7.2(Harvard CMT)级地震.震中位于台湾南部滨海之南海次板块与菲律宾海板块碰撞引发造山作用生成的海洋增生楔内, 这次地震是该区域百年来震级最大的地震.我们利用中国数字地震台网(CSDN)和美国地震学联合研究所(IRIS) 提供的上地幔及远场范围宽频带P波垂向记录资料,基于点源和有限断层模型进行波形拟合反演,获得这次地震的震源机制解并给出了震源破裂过程.反演结果表明,本次地震为东倾正断层兼小幅度走滑破裂事件, 断层面走向为341.5°,倾角为77.9°,震源深度6 km.所得正断层震源机制解表明,地震可能与板块的拆离(break-off)作用引发的在台湾造山带局部存在伸张作用力有关.  相似文献   

7.
丽江7.0级地震的余震震源参数研究   总被引:6,自引:2,他引:6  
本从PDR-2数字化近源(6.2km≤△≤42km)台网记录的丽江余震中初选了74个地震,初定了震中位置,震中方位角。用相应的台网数据处理技术,研究了丽江地震序列的体波谱。对震级2.5≤M≤5.7、地震矩21.40≤longM0≤23.28的地震,得出了丽江地区地震系列的震源参数;以及P波、S波的logM0与Md的关系式分别为:logM0^p=0.62Md+19.93;logM0^s=0.59M  相似文献   

8.
1995年5月2日乌苏南发生Ms5.8级地震1995年5月2日19时48分09秒在新疆乌苏南发生Ms5.8级地震。震中位于λE84°40’,ψN43°49’;震源深度29km;震中烈度Ⅵ度。地震发生后,新疆维吾尔自治区地震局局长石鉴邦率领考察人员,连...  相似文献   

9.
大同─阳高2次地震前后震源应力场的变化过程   总被引:1,自引:0,他引:1  
利用1989、1991年大同-阳高两次地震前后几年的地震记录资料,详细分析了其震源应力场的变化,结果表明,6.1级地震前震源应力场中两个主应力轴的方向曾发生逆转,主压应力袖逆转时间约10个月,主张应力轴逆转时间为2个月。6.1级主震前4个月,两个主应力轴的方向、仰角都恢复到正常状态,且与华北区域应力场的特征某本一致,而1991年5.8级地震前却没有出现上述现象。说明大同-阳高2次地震是在同一震源应力场作用之下孕育、发展的,亦说明5.8级地震是6.1级地震的晚期强余震。指出山西地震带6级以上地震的孕育发生似是在华北区域应力场的作用之下完成的。  相似文献   

10.
1995年7月20日在北京西北的怀来盆地发生了一次ML4.1地震.这次地震震中位于40.326N,115.448E,震源深度5.5km.在此主震之后该地区微震活动变得十分活跃.中-欧合作怀来数字地震台网记录并精确定位了这一地震序列.以8次余震的记录作为经验格林函数提取了ML4.1地震的震源时间函数,并通过叠加得到了信噪比较高的平均结果.结果表明,这次ML4.1地震由一强一弱两次事件组成.各个台站的震源时间函数显示出明显的地震多普勒效应.用试错法得到了ML4.1地震的第一次事件的破裂长度为0.44km,破裂速度为4.0km/s;第二次事件破裂长度为0.25km,破裂速度3.0km/s.两次事件的破裂传播方向与破裂面走向的夹角(逆时针为正)分别为140和90,两次事件相距0.57km,第二次破裂发生于第一次破裂开始之后0.09s.用单个经验格林函数提取了怀来盆地ML4.1地震序列中另外13次ML2.1地震的震源时间函数.结果表明,这些小震均由单次事件组成,震源时间函数宽度为0.05~0.16s.用远场地动位移频谱测量法得到了0.9ML4.1的25次地震的地震矩、应力降和破裂半径.地震矩和应力降都呈现出随震级而单调递增的规律性变化.在0.9ML2.4范围内,求得的破裂半径与震级没有显示出明显的相关性,可以认为,在这样小的震级范围内用本文所用资料已无法准确分辨小震的破裂尺度.   相似文献   

11.
Samples of all eighteen of the known C2 chondrites have been analyzed thermomagnetically. For eleven of these, initial Fe3O4 content is low (generally <1%) and theJs-T curves are irreversible. The heating curves show variable greater (up to 10 times) than it is initially. This behavior is attributed to the production of magnetite from a thermally unstable phase — apparently FeS. Four of the remaining seven C2 chondrites contain Fe3O4 as the only significant magnetic phase: initial magnetite contents range from 4 to 13%. The remaining three C2 chondrites contain iron or nickel-iron in addition to Fe3O4. These seven C2 chondrites show little evidence of the breakdown of a thermally unstable phase.  相似文献   

12.
地震孕育、发生、发展动态过程模拟系统   总被引:6,自引:0,他引:6       下载免费PDF全文
  相似文献   

13.
Laboratory infrared absorption spectral measurements of CF2Cl2 in the 10.8 m band have been performed. Doppler limited resolution has been achieved using semiconductor tunable lasers. The line strength and the self and pressure broadening rates have been measured for the 918.562 and 918.621 cm–1 lines. The results are used for considerations on the application of high resolution spectroscopy to the measurement of atmospheric CF2Cl2.  相似文献   

14.
15.
The UV/H2O2 is one of the popular techniques in the advanced oxidation processes (AOPs) and has been applied in the wastewater treatment during recent two decades. UV exposure on the H2O2 generate highly reactive hydroxyl radicals (OH?), which are used to degrade organic contaminants through oxidation processes in wastewater. This present study involves the estimation of hydroxyl radical rate constants of methyldiethanolamine (MDEA) mineralization at different temperatures by using UV/H2O2 in aqueous solution. Laboratory experiments have been conducted and the profile of MDEA mineralization has been established. The hydroxyl radical rate constants and the activation energy of mineralization process have been calculated. The estimated hydroxyl rate constants and the activation energy are in good agreement with those reported in the literature.  相似文献   

16.
By using the diamond-anvil pressure cell coupled with laser heating, Ca2GeO4 in the K2NiF4-type structure has been found to decompose into the mixture Ca3Ge2O7 plus CaO at pressures greater than 200 kbar and at about 1000°C, and the same type of structure for Ca2MnO4 has been found to decompose into the mixture CaMnO3 (perovskite) plus CaO at pressures greater than 100 kbar and at about 1400°C. The decomposition product of Ca3Ge2O7 is a new compound which is isostructural with Sr3Ti2O7 and has the lattice parameters of a = 3.72 ± 0.01 and c = 19.32 ± 0.05 A? at room temperature and 1 bar pressure. The results of the study of Ca2GeO4 and Ca2MnO4 (both with the K2NiF4-type structure) strongly support the view that compounds possessing the K2NiF4-type structure are unstable relative to corresponding mixtures possessing the perovskite and rocksalt structures. It is concluded that, in the earth's mantle, the K2NiF4-type Ca2SiO4 would ultimately decompose into the mixture CaSiO3 (perovskite) + CaO or would otherwise transform to other as-yet-unknown phase(s), and that the mixture of MgSiO3 (perovskite) + MgO (the post-spinel phase of Mg2SiO4) would not adopt the K2NiF4-type structure.  相似文献   

17.
The properties of the seismic low-velocity zone are consistent with incipient melting of mantle peridotite. Vapor-absent melting of amphibole-peridotite has been used to model the low-velocity zone, but evidence that CO2 exists in the upper mantle indicates that peridotite-CO2-H2O would be a better model. The divariant solidus surface for peridodite-CO2-H2O is traversed by a series of univariant lines marking the intersections of divariant subsolidus reactions involving dolomite or magnesite, amphibole, or phlogopite (other hydrous minerals are neglected in this treatment), or combinations of these. The vapor phase compositions are buffered to specific values, which limits the range of vapor compositions that can coexist with peridotite at various pressures. Below about 30 kbar, the vapor phase is buffered by the melting of amphibole-peridotite, with composition ranging from H2O to high CO2/H2O. Above about 25 kbar, the vapor phase is buffered by the melting of dolomite-peridotite, with composition ranging from CO2 to high H2O/CO2 at pressures above 30 kbar. The buffered curve for phlogopite-peridotite intersects the dolomite-peridotite curve, generating another line for phlogopite-dolomite-peridotite; the strong buffering capacity of dolomite forces the vapor on this line to high H2O/CO2. Near the buffered curve for the solidus of partly carbonated peridotite there is a temperature maximum on the peridotite-vapor solidus surface. On the CO2 side of the maximum, above 26 kbar, CO2/H2O is greater in liquid than in vapor; on the H2O side of this maximum, and at all pressures below 26 kbar, CO2/H2O is greater in vapor than in liquid. The suboccanic low-velocity zone is caused by incipient melting of amphibole-peridotite in the presence of vapor with high CO2/H2O, with generation of forsterite-normative liquid. The subcontinental low-velocity zone, where present, is probably caused by incipient melting of dolomite-peridotite, or phlogopite-dolomite-peridotite, either with H2O-rich vapor or without vapor, with the generation of CO2-rich, alkalic, SiO2-poor liquid (larnite-normative) that in extreme conditions may be carbonatitic.  相似文献   

18.
A brief report is made of current laboratory investigations on phase relations among olivine, pyroxene, anorthite, magnetite, tridymite, liquid and gas in the system Mg2SiO4-CaAl2Si2O8-FeO-Fe2O2-SiO2 over a wide range of oxygen partial pressures. Courses of fractional crystallization under various conditions of oxygen partial pressure are depicted using an anorthite saturation diagram. Starting with a basalt-like composition in the system, fractional crystallization at a moderate oxygen partial pressure (10 atm.) results in an andesite-like residual liquid of composition 55 SiO2, 14 iron oxide, 6 MgO, 9 CaO, 16 Al2O3 at a temperature of 1155°C. With fractional crystallization in a closed system, the end liquid approaches the composition of 45 SiO2, 38 iron oxide, 6 CaO and 11 Al2O3, at a temperature of 1050°C and oxygen partial pressure of about 10?12 atm. The andesitic final liquid in this system would be expected to further differentiate toward dacitic and rhyolitic compositions if alkalies and water were present in the system. On the basis of these studies, the derivation of liquids of andesitic, dacitic or rhyolitic composition from primary basalts by fractional crystallization seems entirely possible if the oxygen partial pressure is maintained at a moderate or high level.  相似文献   

19.
20.
A spectral imager specifically designed to measure the O+(2P-2D) emission in the thermosphere during twilight has been constructed and tested in Toronto (43.8°N, 79.3°W), and found to show promise for long-term and campaign-mode operations. A modification of the mesopause oxygen rotational temperature imager (MORTI), it consists basically of a narrow-band interference filter (0.14 nm bandwidth) to separate wavelengths as a function of off-axis angle, a lens to focus the spectrum into a series of concentric rings, and a focal plane array (CCD) to record the spectral images in digital form. The instrument was built with two fields of view, one for the zenith and one for 20° above the horizon, movable to track the azimuth of the Sun, in order to provide appropriate data for inversion. Data gathered during June 1991 provided measurements of the column-integrated emission rate with a precision of about 3%. An atomic oxygen profile was deduced that showed good agreement with that predicted by the MSIS-90 model atmosphere. Geomagnetically induced variations of the O+ lines, calcium spectra resulting from meteor showers, and OH nightglow were also observed.  相似文献   

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