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1.
塔里木油田碳酸盐岩储层埋藏深,地震资料主频低,走滑断裂断距小,断层地震反射特征不清楚,识别解释难度大.本文基于连续小波变换,提出一种识别深层-超深层碳酸盐岩走滑断裂方法.通过井震标定和地震正演模拟确定走滑断裂敏感频段,利用连续小波变换方法对断裂敏感频率进行筛选加权,突出断层地震反射特征,提高地震资料对次序级走滑断裂的识别能力.ZG8井区实际资料应用表明:经过本文方法处理后的地震数据与常规数据相比,剖面上走滑断裂的断点特征更清楚,平面上提取的相干属性对次序级断裂的刻画更可靠清晰,有利于本区块走滑断裂的综合解释研究以及断溶体的识别刻画.  相似文献   

2.
海阳断裂是胶东半岛NE向牟平 -即墨断裂带东部一条规模较大的断裂 ,尽管晚更新世以来该断裂的地表断错活动总体上已基本停息 ,但东石兰沟段在晚更新世晚期以来仍有断错地表的活动。最后一次断错地表的活动发生在距今 3 7~ 1 2万年 ,但接近 1 2万年。地表破裂长度约6 5km ,活动段长度 8km。地表断错以走滑活动为主 ,可见最大倾滑位移 0 2m ;根据断层擦痕侧伏角推测最大水平位移 1 13m。最后一次断错地表的活动若以距今 1 2万年计算 ,则最大平均倾滑速率为 0 0 17mm/a ;最大平均右旋走滑速率为 0 0 94mm/a。野外观测到该活动段的断错活动表现为突发断错 ,根据地震地表破裂参数、活动段长度与地震的关系 ,估计其最大潜在地震为 6 级  相似文献   

3.
<正>为了研究龙日坝断裂带在青藏高原东缘应变分配中的作用和分析平行走滑断裂带是否会像2008年汶川8.0级地震造成两条平行断裂的共同破裂,开展了龙日坝断裂晚第四纪滑动速率和古地震序列的详细定量研究。野外调查表明,龙日坝断裂带位于龙门山以西约200 km,与龙门山断裂带大致平行,它由两条近平行的断裂(毛尔盖断裂和龙日曲断裂)组成。其中毛尔盖断裂主要沿着毛尔盖河和羊拱沟的北侧基岩山坡展布,发育断错山脊和断错水系,其晚第四纪活动表现为右旋走滑;龙日曲断裂主要沿龙日曲河和雀儿  相似文献   

4.
采用地表地质调查、地貌调查、建筑物震害调查方法,结合震源机制解及余震分布、地震烈度图,初步探讨了广西北流M_S 5.2地震发震构造特征。研究结果表明:广西北流M_S 5.2地震发生在NW走向的石窝断裂和NE走向的新丰断裂交汇部位,发震构造为石窝断裂;石窝断裂露头平均产状222°∠81°,最新活动性质为具有正断分量的左行走滑断层,最新活动时代为早第四纪;新丰断裂最新运动性质为逆断,最新活动时代为早第四纪;在现今NW向主压应力作用下,石窝断裂发生破裂,发生M_S 5.2地震,同震运动方式以右行走滑为主,余震震中呈NW向分布。极震区建筑物震害调查得出的运动方向与震源机制解显示的同震运动方向一致。  相似文献   

5.
天全-荥经断裂是青藏高原东南缘的1条晚第四纪且活动资料较少的断裂,在2008年汶川M 8.0地震之后,龙门山断裂带西南端未来的地震危险性受到关注。对天全-荥经断裂晚第四纪活动特征的获取有助于理解该区地震危险性的评价。通过遥感影像解译,结合野外调查和断错地貌测量,分析了天全-荥经断裂在荥经下坝村至桂花村切过荥经河河谷晚第四纪地貌区的活动证据。断裂沿线形成冲积扇断错、阶地坎断错和断坎等地貌,并沿断裂发育滑坡。晚第四纪以来断裂以左旋走滑活动为主,其中T2/T2'阶地坎被左旋断错22—24m。利用荥经河阶地与青衣江河流阶地对比,认为该断裂20—40ka以来左旋走滑速率为0.6—1.1mm/a。仍需要从古地震等方面开展工作,来进一步确定天全-荥经断裂的地震危险性。  相似文献   

6.
丽江-小金河断裂是川滇菱形块体内部重要的边界断裂,前人根据其断错地貌特征确定其为左旋走滑断层,并认为其左旋断错了SN向的丽江盆地。本文对丽江-小金河断裂丽江盆地隐伏段开展了浅层地震勘探与钻孔探测,通过地层岩性分析建立跨断层的钻孔联合剖面,揭示丽江-小金河断裂斜穿了丽江盆地,隐伏段整体形式为不对称正花状构造,表现为断展褶皱和逆冲断层,但主断层顶部表现为局部拉张,断错了晚第四纪地层。  相似文献   

7.
巴彦浩特断裂位于阿拉善地块与鄂尔多斯地块相互作用的边界构造带上,其晚第四纪活动特征和古地震数据对全面理解贺兰山周边区域地震构造和地震危险性具有重要意义,为此在研究相对薄弱的巴彦浩特断裂北段开展了断错地貌和古地震槽探研究。观测显示巴彦浩特断裂阿拉善左旗以北段以右旋走滑活动为主兼具逆倾滑,断层西盘相对抬升,在浅表形成半正花状构造组合。年代(56.28±4.04)~(82.2±5.78)ka的冲洪积地貌面上冲沟断错137 m,并在东侧形成断塞塘地貌,估计断层右旋走滑速率为1.67~2.43 mm/a。探槽揭示了3次具有显著地表逆倾滑破裂的强震事件,时间分别为(56.28±4.04)~(55.33±3.04)、(32.79±2.22)~(13.76±1.1)、(13.76±1.1)~(7.86±0.43)ka,逆倾滑量分别为0.44、0.35、0.29 m。与前人在巴彦浩特断裂南段的古地震研究进行对比,可知这3次古地震可能仅为部分事件记录。结合已有研究成果建立了贺兰山周边区域地震构造模型,贺兰山西侧右旋走滑的巴彦浩特断裂强震发震能力不容忽视,贺兰山两侧盆地不同性质断裂系共同构成了阿拉善地块与鄂尔多斯地块的活动边界构造带。  相似文献   

8.
汶川地震地表破裂在东北端从石坎子乡到窝前的运动性质存着从走滑分量略高于倾滑分量到完全为右旋走滑运动的变化过程,倾滑分量在石坎子—平溪段具有逆断性质,在矿坪子及其以北为正断性质,未见挤压变形,窝前完全为右旋走滑运动,地表变形带宽度集中在10m以内;在董家村,地震地表破裂带主要表现为张性裂缝及地堑式负地形,是地震破裂在尾端应力作用下,应变不均一性调节的产物,地表变形带宽度约10~12m;在东河口以北未见地表破裂的证据,推测汶川地震地表破裂带没有穿过流经青川县东河口、关庄、凉水井一带的清水河,东河口一带的构造地貌现象反映了垂直差异性运动,不存在右旋走滑运动的地质地貌证据。在中央断裂东北端断层一侧隆升和另一侧拉张的典型四象限格局成为汶川地震地表破裂的端部表现特征。中央断裂上的汶川地震地表破裂带总长度为240km左右。在汶川地震过程中,沿着中央断裂在地表产生的构造变形在中央断裂的范围内就已经得到了调整,并没有越过中央断裂的范围而传递到以外的地段。  相似文献   

9.
基于川滇地区活动块体划分及断裂构造现有认知,文中构建了包含块体主要边界断裂的二维有限元接触模型,利用1991—2015年长期GPS观测结果,采用"块体加载"方法模拟块体边界带现今的运动,得到了断裂滑动速率和应力分布.结合震源机制解、地震活动性等资料,对川滇地区大型左旋走滑断裂带滑动速率分配、传递与应力转换的关联,局部区域正断型震源机制解的构造机制以及红河断裂南、北段地震活动性差异的可能成因进行了初步探讨.主要结论包括:1)东昆仑断裂带和鲜水河-小江断裂带的左旋走滑由NW向转变为近SN向,断裂强烈转折区吸收了部分走滑分量并转化为应变积累,呈高应力分布特征.2)受小江断裂左旋剪切的影响,红河断裂中南段以右旋走滑兼微弱挤压运动为主,并牵引断裂北段右旋走滑,与金沙江和德钦-中甸断裂共同构成右阶斜列右旋剪切变形带,正断型震源机制解多分布于该变形带的构造拉分区内.3)红河断裂中南段为弱压性,北段呈弱张性,更易破裂,地震活动明显强于中南段.  相似文献   

10.
探究了地震构造区内地震相对震级大小分布或b值系统地取决于断裂类型的假设。因为b值已被证明与应力成反比,我们希望发现b逆断b走滑b正断。我们针对意大利的例子检验这一期望。我们首先建立了地震构造分区模型,它包含10个不同的构造区。然后基于震源机制用初动和全波形的矩张量之和表述每个构造区断裂类型的特征。我们计算了每个构造区的b值,发现逆断层区的b值最低,在0.75~0.81之间,正断层区的b值最高,为1.09,走滑区的b值居中,介于0.9~0.92之间。我们的结果表明,b值作为所有地震危险性评估的一个关键参数,应该根据当地的断裂状态确定。另外,地震构造分区模型中应将b值的变化作为一个输入参数。  相似文献   

11.
The determination of the coefficient of viscosity of eruptive products gives useful elements to the knowledge of possible variations of composition and physical conditions of the magmas.  相似文献   

12.
13.
14.
Geomagnetism and Aeronomy - The magnetic evolution of the active region of the Sun at the level of the photosphere has been studied. Magnetic synoptic maps of the 2007 Kitt Peak Observatory were...  相似文献   

15.
Until recently, the existing data prevented the geophysicists from accurately dating the Bysy-Yuryakh stratum, which outcrops in the middle reach of the Kotuy River, constraining the time of its formation to a wide interval from the end of the Late Cambrian to the beginning of the Silurian. The obtained paleomagnetic data unambiguously correlate the Bysy-Yuryakh stratum to the Nyaian regional stage and constrain its formation, at least a considerable part of it, by the Tremadocian. This result perfectly agrees with the data on the Bysy-Yuryakh conodonts studied in this work and yields a spectacular example of the successful application of paleomagnetic studies in solving important tasks of stratigraphy and, correspondingly, petroleum geology. Within the Bysy-Yuryakh stratum, we revealed a large normal-polarity interval corresponding to the long (>1 Ma) period when the geomagnetic reversals were absent. This result, in combination with the data for the Tremadocian and Middle–Upper Cambrian sequences of the other regions, indicates that (1) the rate of occurrence of the geomagnetic reversals on the eve of the Ordovician Moyero superchron of reversed polarity was at most one reversal per Ma; (2) the superchron does not switch on instantaneously but is preceded by a certain gradual change in the operation conditions of the dynamo mechanism which, inter alia, manifests itself by the reduction of the frequency of geomagnetic reversals with the approach of the superchron. This finding supports the views according to which a process preparing the establishment of the superchrons takes place at the core–mantle boundary.  相似文献   

16.
Резюме Дается вывод формул для вычислений длины хорды, длины и азимутов нормаляных сечений и длины геодезической линии эллипсоида. Применяются тригонометрические функции данных величин и постоянные принятого ргфгргнц-эллипсоида, что является целесообразным при использовании вычислителQjных машин, особенно автоматов. Рабочие формулы рекомендуются в форме (8–11).

Dedicated to Professor František Fiala on His 85th Birthday

Address: Veveři 95, Brno.  相似文献   

17.
Summary A simple model is proposed suitable for studying the effect of the ground layer of the atmosphere, polluted by aerosol, on the albedo. This model is founded on solving the equation of transfer of radiative energy. The numerical results are discussed, particular attention being paid to the analysis of errors due to neglecting the multiple reflection of solar radiation on the aerosol particles. A method which would also include the multiple reflection is proposed, and the conditions under which the presence of the aerosol is responsible for an increase or decrease of the solar radiation balance on the Earth's surface, are analysed.  相似文献   

18.
Summary The author mentions the aims of the World-wide gravity project he established in the Ohio State University in Columbus, in 1950. He outlines the practical procedure of the gravimetric computations of the undulationsN and the vertical deflection components and and emphasizes that only by the global international cooperation and additional gravity observations at sea carried out during the last decade it has been possible to gather to Columbus the needed gravity material. Since there exist still large gravimetrically unsurveyed areas it is of vital significance to study what gravity anomalies are best to be used for these regions. The given figures concerning the accuracy of theN, and , estimated theoretically and obtained in practice, indicate that in the gravimetrically well surveyed parts of the world like in Europe and the United States we can get gravimetrically on basis of existing gravity material theN-values with accuracy of about 5–10 meters, and and with the accuracy of about 1. The geoid undulationsN are already computed in Columbus for more than 6000 points of the northern hemisphere. The sample maps show the interesting geoid of Europe and vicinity between the latitudes 60° and 30° and longitude 5° W and 30° E, drafted on basis of more than 1000N-values computed at the corners of 1°×1° squares. It is interesting to realize that the geoid undulations in all this area are positive, the extreme values being between 40 and 50 meters. The geophysical significance of the geoid maps of this kind is pointed out.  相似文献   

19.
Summary The maintenance of the axisymmetric component of the flow in the atmosphere is investigated by means of a steady-state, quasi-geostrophic formulation of the meteorological equations. It is shown that the meridional variations in the time-averaged axisymmetric variables can be expressed as the sum of three contributions, one being due to the eddy heat transport, another to the eddy momentum transport, and a third to the convective-radiative equilibrium temperature which enters the problem through the specification of a Newtonian form of diabatic heating. The contributions by the large scale eddies are evaluated through the use of observed values for the eddy heat and momentum transports.The contributions from each of the three forcing mechanisms to the temperature and zonal wind fields are invstigated individually and found to be of about equal importance. The sum of the three contributions are also presented for the temperature, the zonal wind, the stream function associated with the mean meridional circulation and the corresponding vertical motion. Although the results fail to reproduce the main observed features of the lower stratosphere, they are found to be in good agreement with observations in the middle latitude troposphere. At any pressure level, for example, the computed mean zonal wind has a jet-like profile and the axis of the jet is found to slope to the south with height, as observed in the atmosphere.Based in part on a thesis submitted by the first author as partial fulfillment of the requirements for the Ph.D. degree at the University of Michigan. — Publication No. 194 from the Department of Meteorology and Oceanography, The University of Michigan.  相似文献   

20.
Atmospheric temperature and humidity fields as well as information on other meteorological parameters are nowadays retrieved from radiance measurements recorded by operational meteorological satellites. Up to now, the inversion procedures used only take into account crude information on the topography of the Earth’s surface. However, the applied radiative transfer codes have to consider the Earth’s surface as the lower boundary of the atmospheric model and, therefore, need a more precise mean elevation and a classification of the roughness of the Earth’s surface. The influence of the topography of the Earth surface on retrieved temperature profiles is studied by using a physico-statistical inversion method. An objective analysis is made of the more precise mean elevation and derivation of roughness parameters using a new high-resolution digital elevation model (DEM) with a resolution of 500 m×500 m. By means of a geomorphological process and a newly developed topography rejection test, areas with a high surface roughness are localized and singled out. The influence of topography on the retrieved temperature profiles is illustrated by case studies. Changes are found predominantly in areas with a high variation of topography. Using the new high-resolution DEM and the topography rejection test, the geographical position of the calculated temperature profiles tends to be shifted towards areas with a small vertical variation of topography. The mean elevation determined by the new elevation model better characterizes the area observed. Hence, the temperature profiles can be calculated down to lower atmospheric levels. Furthermore, a guess profile better describing the atmospheric situation is selected by the more precise elevation. In addition, the temperature profiles obtained near the coast are improved considerably by the more precise determination of the surface property ‘sea’ and ‘land,’ respectively. Integration of an independent physical information such as topography leads, on average, to a slight improvement of the results of the physico-statistical inversion procedure. In some cases, however, significant improvements have been achieved regarding the desired accuracy of temperature profiles of the order of 1 K. In future, the spatial resolution of new high-resolution sounding instrumentation on the next generation of operational meteorological satellites will be increased. To exploit the resolving power of this new instrumentation, the different variation of the topography of the Earth surface, especially in regions with a high variation of topography, can be taken into account more precisely by using a high-resolution DEM.  相似文献   

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