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采用波形反演方法对青藏高原地区震中距8°-38°范围内的宽频带炸波波形进行拟合,研究该地区上地幔平均速度结构以及上地幔纵、横波速度的横向不均匀性结果表明青藏高原地区的平均地壳厚度约为68km,上地幔盖层平均厚度约为30－40km,速度约为8.10km／s雅鲁藏布江附近地壳厚度最大,约80km,相应的上地幔Pn速度为8．15km／s左右,青藏高原中部地区的地壳平均厚度约68-70km．位于拉萨地块北部的羌塘地块S波速度相对较低,其地壳和上地慢的平均S波速度分别比拉萨地块低1％和2％以上34°N以北,90°E附近的区域存在明显的上地幔P波低速异常区,P波的平均速度小于7．8km／s据此结果及前人工作,推断印度板块的俯冲可能以雅鲁藏布江缝合带附近为界,青藏高原巨大的地壳厚度是由于欧亚板块碰撞造成地壳缩短与增厚引起. 相似文献
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1303年在山西洪洞附近发生的8级巨大地震, 是中国根据现存较为详细的文献记载史料所确定的最早的一次8级地震。 这次地震距今已有700多年的历史, 而地震所在区域至今仍有持续不断的小地震活动。 本文根据地震破裂区1981年至2013年的中小地震精定位地震目录, 采用震源断层面拟合方法, 反演得到了1303年山西洪洞地震的震源断层面参数: 走向19.3°、 倾角88.5°、 滑动角-170.0°。 断层面长75.5 km, 宽26.2 km, 深度为地下11.12 ～37.35 km。 将地震破裂区的地震精确定位资料以近东西向的洪洞断裂为界划分为地震北段和地震南段, 分段进行地震震源断层拟合, 反演得到洪洞地震北段震源断层面参数: 走向13.7°、 倾角76.6°、 滑动角-157.6°。 断层面长32.7 km, 宽21.7 km, 深度为地下11.97～32.86 km; 南段震源断层面参数: 走向20.3°、 倾角87.1°、 滑动角-154.6°。 断层面长45.9 km, 宽16.6 km, 深度为地下9.32 km～25.50 km。 无论是分段还是不分段, 反演得到的洪洞地震震源断层均是右倾的近直立断层, 属于右旋走向滑动性质。 分段计算得到的地震北段震源断层深度比南段更深, 将反演得到的震源断层与临汾盆地深部构造最新研究成果进行了分析对比, 北段震源断层深度及倾角大小与深地震剖面推测得到的深大断裂几乎相同。 震源断层在地表的投影与洪洞地震的高烈度区能够较好地对应。 相似文献
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The spectral study of the Bouguer anomally map of Central India suggests an uplifted crust-mantle interface under the Mahandi graben. This study has delineated three subsurface levels of anomalous masses at the respective depths of 23 km, 8 km, and 2 km apparently representing the Moho, an intermediate discontinuity in the sialic part of the crust and the basement, respectively. Model study of the Bouguer anomaly along a profile suggests a typical continental graben type subsurface structure with a low density depression in the sialic part of the crust between 8 and 18 km supported by an elevated upper mantle of intermediate density (3.4 g/cm3) varying in depth from 25 km to 55 km. The depths of the inferred interfaces in case of Bundelkhand granite are 32 km, 11 km, and 1.5 km, which might represent the Moho, the base of intruded granite massif, and some shallow compositional variation. Similar studies in case of Vindhyan basin have brought out three discontinuities at the respective depths of 16 km, 6–4.5 km, and 2.4 km. The first horizon at the depth of 16 km probably represents the interface between the granitic and the basaltic part of the crust. The 6–4.5 km is the depth of the basement, with the 2.4 km interface separating Bijawar rocks from Vindhyans wherever they are present. A generalized inversion of a profile across a positive belt of Bouguer anomaly representing the subsurface Bijawar rocks support the above result. 相似文献
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利用Hypo2000+HypoDD联合定位方法,基于35个科考台站和四川测震台网记录资料,对2013年6月25日至2014年12月31日发生的芦山M_S 7.0地震余震序列进行重定位。重新定位后,EW、NS和UD向平均误差分别为0.141 km、0.143 km、0.147 km,平均到时残差0.066 s,震源深度优势分布范围8—18 km。定位结果显示,芦山地震余震呈带状分布,主要分布在大邑—名山断裂和双石—大川断裂之间,沿SW方向,长度约40 km。 相似文献
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本文是1986年古雷—石城剖面及嵩口—宜城剖面深地震测深资料的初步研究结果。 对古雷—石城的纵剖面资料,分析了震相特征,共识别出五个波组:P_2、P_3~0、P_4~0、P_5~0及P_n(P_n~0)。通过对波的走时反演,正演拟合和理论地震图方法等计算,得到了该区地壳与上地幔结构模型。 古雷—石城地区地壳具有多层结构,并可划分为上、中、下三层。古雷炮点给出的厚度分别为1.0km、15.7km、12.8km,地壳平均速度为6.29km/s,深度为29.5km,上地幔顶面P_n波速度为7.83km/s。石城炮点给出厚度分别为1.8km、18.3km、12.4km。地壳平均速度为6.29km/3,深度为32.4km,土地幔顶面P_n速度为8.00km/s。 在中地壳下部存在一低速层,其厚度为2.8km,速度为5.85km/s。根据其它研究结果,初步判断低速层介质是半熔融物质组成。 测区内横向变化比较强烈。从东向西有长乐—诏安、政和—海丰和邵武—河源三个大断裂穿过该区,并且都深切至莫霍面;在漳州盆地之下莫霍面隆起约3km,戴云山区下莫霍面凹陷近2km;永安—梅州莫霍面隆起接近3km。莫霍面分布显示出从东南向西北逐渐加深。 宜城—连城—嵩口非纵剖面显示了莫霍面在两处有明显断错,错距约2km邵。表明昭武—河源断裂是切割莫霍面的深大断裂。 相似文献
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Mantle-lithosphere bodies in the Alboran crustal domain (Ronda peridotites, Betic-Rif orogenic belt)
M. Torn E. Banda V. García-DuenÜas J.C. Balany 《Earth and Planetary Science Letters》1992,110(1-4):163-171
Geological and geophysical data are used to demonstrate the existence of intracrustal high-density/high P-wave velocity bodies in the western Betics. These bodies appear to correspond to buried peridotites similar to those that outcrop in the Ronda area. A gravity study shows how the gravity field is mainly the result of a combined effect of crustal thinning and the presence of ultramafic bodies. The size of the buried high-density body, as interpreted from gravity and seismic results, shows maximum dimensions of about 40 km in length (NNW-SSE), about 8 km in thickness, and a lateral extension (ENE-WSW) of about 70 km. The thinning of the crust from 32–35 km to 20–22 km takes place in a narrow area less than 35 km wide. Our results are compatible with an interpretation in terms of an unrooted peridotite slab. Dismembering of an initial slab of ultramafic rocks is a possible consequence of the extensional regime that originated the Alboran basin. 相似文献
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Dr. Heinrich Faust 《Pure and Applied Geophysics》1963,56(1):194-202
Zusammenfassung Oberhalb der Nullschicht addieren sich Druck und Temperatur hinsichtlich ihrer Wirkung auf die Dichte. Es existiert in etwa 11 km Höhe eine Horizontalfläche maximaler Dichteabnahme vom Hoch zum Tief. Der Luftdruck in der Schicht maximalen Horizontalgradienten des Drucks in etwa 8 km ist ein Maß für die Intensität eines Druckgebildes. Die Stärke der Korrelation zwischen dem Druck in 8 km und der Dichte in 11 km ist somit ein maß für die Stärke der Nullschichtvorgänge.
Diese Arbeit wurde unterstützt vom US-Department of the Army, European Research Office, unter Kontrakt Nr. DA-91-591-EUC 2847. 相似文献
Summary The large scale vertical motions in high and low pressure systems are, in the mean, reversed in the null layer, connected with the upper-tropospheric wind maximum layer (about 10 km altitude). Above the null layer pressure and temperature influence the air density in the same sense; below it their influence upon the air density is opposite. In an altitude of 11 km (middle latitudes) there exists a horizontal surface with a maximum of density-decrease from high to low pressure areas. Typical for the intensity of a pressure system is the pressure in the layer of maximum horizontal pressure gradient in an altitude of 8 km. The strength of the correlation between pressure in 8 km and density in 11 km is proportional to the strength of the processes in the null layer (Fig. 5a-d). The non-gradientic mass flow to high pressure areas in the null layer is great in high latitudes (high Coriolis parameter) and in winter (high meridional temperature gradient). In a low in formation more potential energy is available in winter, which can be transformed in kinetic energy of the winds in the null layer.
Diese Arbeit wurde unterstützt vom US-Department of the Army, European Research Office, unter Kontrakt Nr. DA-91-591-EUC 2847. 相似文献
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利用中国科学院国家空间科学中心廊坊站(40.0°N,116.3°E)钠荧光多普勒激光雷达2011年至2013年共约82 h的钠原子数密度和垂直风观测数据,分析了廊坊地区中间层顶区域大气重力波耗散引起的钠原子输送特征.分析得到,90~100km处重力波耗散引起的平均钠原子垂直通量整体为负,钠原子向下输送,在93 km处达到最大负值-1.47×10~8m~(-3)m·s~(-1),85~90km处平均钠原子垂直通量为正,钠原子向上输送,但通量值随高度递减.钠原子垂直通量方向在90km处发生转变,垂直通量随高度的变化造成钠原子汇聚,汇聚效应引起的平均钠原子产生率最大值在91km处达到了1.40×10~8m~(-3)/h,该值超过了相同高度上模式计算流星烧蚀注入引起的钠原子产生率峰值,说明重力波耗散对钠层结构的形成具有重要影响.与美国SOR和Maui观测结果相比,平均钠原子产生率峰值大小相近,但出现高度不同,说明大气重力波耗散引起的物质输送具有显著的地域变化特征.研究结果可为大气物质输送理论的完善以及大气金属层物理模式的改进提供观测事实参考. 相似文献
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通过跨银川断陷盆地,完成了一条长68.9 km的高分辨深地震反射探测剖面,首次获得了银川盆地地壳精细结构、地堑型断陷盆地深部断裂系（黄河断裂、银川断裂、贺兰山东麓断裂）特征及深浅构造关系.结果表明：银川断陷盆地上地壳为双程走时8 s（深度约20 km）反射面以上的区域,上地壳上部地层层位丰富,地层分段连续性较好,上地壳下部地层分层特征不明显,地质构造简单;下地壳(8～13 s)反射能量较弱,反射同相轴不明显;下地壳下部壳幔过渡带（13 s附近）由一组能量较强、持续时间较长（1.5 s）的反射波组组成,厚度约4.5 km.芦花台断裂、银川断裂分别于12～12.5 km、18～19 km深处交汇于贺兰山东麓断裂,贺兰山东麓断裂于28～29 km深处交汇于黄河断裂,黄河断裂为错断Moho面的深大断裂,银川地堑为以黄河断裂为主,其他断裂为辅组合而成的负花状构造.根据贺兰山东麓断裂和银川断裂的相互关系,认为贺兰山东麓断裂对1739年平罗—银川8级地震起主要控制作用. 相似文献
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S波速度结构能够反映地球介质的物性差异,是地壳内低速区结构特征判别的重要依据.本文尝试利用空间自相关法(SPAC法)从地震台站微动信号的垂直分量中提取瑞利波相速度频散曲线,通过对频散曲线的反演获得地下介质的S波速度结构.以国家数字测震台网8个宽频带地震台站的实测微动数据为例,采用SPAC方法获得了首都圈地区北京附近约30 km 深度范围内的一维S波速度结构.结果表明,该区结晶基底埋深较浅约2 km;分别在5~8 km 和12~16 km 深处发育S波低速层;8 km 和 20 km 处是S波速度差异较大的速度分界面.这一结果与以往地震学及人工地震探测结果较为吻合,表明SPAC法估算地壳S波速度结构是可行、有效的. 相似文献
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为了更好地确定2017年8月8日九寨沟M_(S )7.0地震震源深度其发震机理,利用四川、甘肃和青海区域地震台网的观测波形数据,采用多种方法研究了此次地震的震源深度。首先,采用gCAP方法反演了九寨沟M_(S )7.0地震的震源机制解和矩心深度,结果显示,节面Ⅰ走向243°/倾角87°/滑动角-158°,节面Ⅱ走向151°/倾角68°/滑动角-3°,矩震级为M_(W )6.5,矩心深度为8 km;然后,采用ISOLA近震全波形方法反演了此次地震的震源机制解,反演结果与gCAP方法结果相差不大,矩心深度为7 km;最后,通过sPn震相与Pn震相之间的走时差测定此次地震初始破裂震源深度,结果显示深度约为12 km。研究表明,九寨沟M_(S )7.0地震的矩心深度为7—8 km,初始破裂深度约为12 km。 相似文献
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Hekla and Torfajökull are active volcanoes at a rift–transform junction in south Iceland. Despite their location next to each other they are physically and geologically very different. Hekla is an elongate stratovolcano, built mainly of basaltic andesite. Torfajökull is a prominent rhyolitic centre with a 12-km-diameter caldera and extensive geothermal activity. The scope of this study is to examine the propagation of body waves of local earthquakes across the Hekla–Torfajökull area and look for volumes of anomalous S-wave attenuation, which can be evidence of magma chambers. So far the magma chamber under Hekla has been modelled with various geophysical means, and its depth has been estimated to be 5–9 km. A data set of 118 local earthquakes, providing 663 seismic rays scanning Hekla and Torfajökull, was used in this study. The major part, 650 seismograms, did not show evidence for S-wave attenuation under these volcanoes. Only six seismograms had clear signs of S-wave attenuation and seven seismograms were uncertain cases. The data set samples Hekla well at depths of 8–14 km, and south part of it also at 4–8 km and 14–16 km. Western Torfajökull is sampled well at depths of 4–14 km, eastern and southern Torfajökull at 6–12 km. Conclusions cannot be drawn regarding the existence of magma beyond these depth ranges. Also, magma volumes of smaller dimensions than about 800 m cannot be detected with this method. If a considerable molten volume exists under Hekla, it must be located either above 4 km or below 14 km. The former possibility seems unlikely, because Hekla lacks geothermal activity and persistent seismicity, usually taken as expressions of a shallow magma chamber. An aseismic volume with a diameter of 4 km at the depth of 8 km in the west part of Torfajökull has been inferred in earlier studies and interpreted as evidence for a cooling magma chamber. Our results indicate that this volume cannot be molten to a great extent because S-waves travelling through it are not attenuated. Intense geothermal activity and low-frequency earthquakes are possibly signs of magma in the south part of Torfajökull, but a magma chamber was not detected there in the areas sampled by this study.Editorial responsibility: T. Druitt 相似文献
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We invert teleseismic relative residuals recorded in the Thessaloniki seismological network, for the crustal and upper mantle structure beneath Chalkidiki (Northern Greece) where extension is observed to have occurred since Eocene time. After conducting several tests to insure the reliability of the results, a low-velocity anomaly (5–8%) is observed which is located beneath Chalkidiki for the top two layers (0–35 km and 35–85 km); this anomaly is probably related to the fact that the crust is thicker here than beneath the neighboring basins. For the two other layers, with depths between 85 and 145 km and between 145 and 205 km, relatively low velocities (3–5%) are observed beneath the Thermaico Gulf and the Kavala Basin. These results are compared with Lyberis's (1985) [8] calculated shallowing of the isotherms due to extension and thinning of the lithosphere. We conclude that the velocity anomalies that we observe are likely to be due to the intrusion of hot material from the asthenosphere into the gap in the extended lithosphere. 相似文献
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采用双差层析成像方法,对2014年3月27日M4.7和3月30日M4.5秭归震群重定位显示:0～5 km深度层P波高速区分布在仙女山断裂北中段和九畹溪断裂北段,天阳坪断裂一带为低速区;8 km深度层高速区分布在九畹溪断裂东侧,仙女山断裂较低;11 km层高速区仅分布在高桥断裂和周家山—牛口断裂之间地带。在地震集中区的下方(即8～12 km处)存在分布较为稳定的低速区,较大地震事件主要分布在高速区或高低速区交界地带,低速区内则很少有地震分布。局部高速体的存在为岩石发生瞬间破裂提供了物质基础,其与低速体间的梯度带是发震构造常发育的区域。研究区内的仙女山断裂北段、九畹溪断裂正是在该梯度带内发育的两条活动断裂。本地震序列的自地表至5 km和5～10 km深度范围内均有大量破裂存在表明,浅层地震仍在水库渗透范围内,而深部地震则与流体渗透无关。此次地震活动同时存在水库诱发地震和构造地震存在。 相似文献
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《Journal of Geodynamics》1999,27(4-5):567-583
Upper mantle P and S wave velocities in the western South America region are obtained at depths of foci from an analysis of travel time data of deep earthquakes. The inferred velocity models for the Chile–Peru–Ecuador region reveal an increase of P velocity from 8.04 km/s at 40 km to 8.28 km/s at 250 km depth, while the S velocity remains almost constant at 4.62 km/s from 40 to 210 km depth. A velocity discontinuity (probably corresponding to the L discontinuity in the continental upper mantle) at 220–250 km depth for P and 200–220 km depth for S waves, with a 3–4% velocity increase, is inferred from the velocity–depth data. Below this discontinuity, P velocity increases from 8.54 km/s at 250 km to 8.62 km/s at 320 km depth and S velocity increases from 4.81 km/s at 210 km to 4.99 km/s at 290 km depth. Travel time data from deep earthquakes at depths greater than 500 km in the Bolivia–Peru region, reveal P velocities of about 9.65 km/s from 500 to 570 km depth. P velocity–depth data further reveal a velocity discontinuity, either as a sharp boundary at 570 km depth with 8–10% velocity increase or as a broad transition zone with velocity rapidly increasing from 560 to 610 km depth. P velocity increases to 10.75 km/s at 650 km depth. A comparison with the latest global average depth estimates of the 660 km discontinuity reveals that this discontinuity is at a relatively shallow depth in the study region. Further, a velocity discontinuity at about 400 km depth with a 10% velocity increase seems to be consistent with travel time observations from deep earthquakes in this region. 相似文献
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本文主要叙述利用近年来北京及其附近地区八次工业爆破的观测资料,同时也利用了一部份天然地震的资料来研究北京-天津-唐山-张家口地区地壳结构的结果,采用了工业爆破中的58个观测点和天然地震的54个观测点的数据,得到了本区的三层地壳模型和地壳厚度。 地壳的平均厚度分布各地区不很一致;北京及其东南地区为35±1.5公里,北部地区为37±1.0公里,西部地区为39±1.5公里,地壳介质中的纵波和横波的平均速度分别为6.23±0.03公里/秒和3.55±0.05公里/秒,上地幔顶部介质的平均速度为7.98±0.13公里/秒和4.60±0.03公里/秒。 相似文献
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在频域使用多窗口(Multitaper)方法来计算月球正面四个形成于不同历史时期月海区(Smythii, Crisium, Imbrium, Orientale)的重力地形导纳,然后将其与月球弹性岩石圈的理论导纳模型相比较,由最小二乘法得出四个月海区的月球岩石圈的平均弹性厚度约为8 km,月壳的厚度分别为：Smythii 盆地,72 km; Crisium 盆地 70 km;Orientale 盆地 60 km;Imbrium 盆地57 km.随着月球的演化,月壳厚度呈现变厚的趋势. 相似文献
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INTRODUCTIONAnMS6 2earthquakeoccurredon 1 0Jan .1 998ontheborderofZhangbeiandShangyicountriesofHebeiProvince .TheearthquakewasnamedtheZhangbei_Shangyiearthquake .Theepicenterislocatedintheregion ,whichiscoveredwithbasaltandthereisnoactivefaultonthesurface .Aftertheearthquakeoccurred ,manyscholarsstudieditsseismogenictectonicsandfocalcharacteristicsinaspectsofactivestructure ,aftershockdistribution ,intensitycontour,focalmechanismetc .(XuXiwei,etal.,1 998;XuJie ,etal.,1 998;MaShutia… 相似文献