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1.
对郯庐断裂及其邻区的重磁场资料进行整理和分析,给出了断裂带分段位场特征。结合4条地学断面资料,对郯庐断裂性质、深部地壳构造进行了研究。结果认为,郯庐断裂具有明显的分段性,不同段落重磁场特征不同。以郯庐断裂为界,两侧断裂走向不同:西侧6条断裂走向为东西或近东西向,可看出郯庐断裂东侧是向北东向移动;西侧向西南移动,并以走滑为主的大型左旋平移断裂带。根据深部地壳构造特征,郯庐断裂是一条近于直立、一直延伸并切过莫霍界面的深大断裂带,该断裂地壳结构以破碎为主并表现上宽下窄的特征。根据重力场特征,推断郯庐断裂南部边界到武穴(广济)为止,没有继续南延过长江。 相似文献
2.
沿郯城-庐江断裂带两侧各约500 km内发育的中生代以来白云母花岗岩、二云母花岗岩和A型花岗岩,五大连池、科洛和二克山火山岩带的强碱性富钾火山岩,高87Sr/86Sr值、低εNd值的中新生代玄武岩,沿郯庐断裂带两侧盆地广泛发育的磨拉石建造,稀土元素∑REE,∑LREE,∑LREE/∑HREE从老到新均逐渐增高;郯庐断裂带莫霍面深度明显大于两侧盆地;郯庐断裂带两侧地块的不连续与差异;沿郯城-庐江断裂带展布的华北地台北缘及东缘的高压麻粒岩、NNE向展布的日照、莒南、东海榴辉岩超高压带和安徽张八岭高压蓝片岩带;郯庐断裂带内表现的强烈挤压构造;郯庐断裂带东侧胶辽-苏北黄海负磁异常区不同于周围地质体(正磁异常区)等,所有证据都指示着南起安徽庐江,经山东郯城、黑龙江佳木斯,北至俄罗斯尚塔尔群岛的断裂带及其两侧构造带为-构造碰撞带:郯庐-尚塔尔碰撞带,郯庐-尚塔尔断裂带为碰撞带的缝合线.松辽盆地、华北盆地、苏北盆地等成煤、成油气等矿产的盆地是碰撞的结果.碰撞带的(突出)应力集中区鲁西-胶东超高压带碰撞区、燕山-辽东碰撞区是中国东部地震的高发区.碰撞的主要动力机制为日本海和鄂霍次克海的张开及菲律宾板块的俯冲. 相似文献
3.
郯庐断裂带起源于华北克拉通与扬子板块的汇聚过程中已被多数学者所认同。该断裂带的起源机制，涉及到这两个大陆板块的汇聚方式。可是，对于这一重要问题却长期存在着不同的认识。本文依据郯庐断裂带内部及其两侧前陆上构造与年代学研究成果，综合分析该断裂带的起源机制。郯庐断裂带内部残留的起源期构造为左行走滑韧性剪切带，所获得的白云母40Ar/39Ar同位素年龄为239~217 Ma。华北克拉通边缘的徐淮弧形逆冲-推覆构造，及九江地区扬子板块上的弧形褶皱带，分别为苏鲁造山带、大别造山带点碰撞的产物。郯庐断裂带西侧的华北克拉通边缘，在汇聚过程中呈现为刚性陆块的特征，没有出现大规模的牵引弯曲现象。而东侧的扬子板块前陆构造，在汇聚过程中却明显出现了大规模的牵引弯曲现象。断裂带东侧的张八岭隆起北段，出露了扬子板块上中地壳韧性拆离带，其中所获得的白云母40Ar/39Ar同位素年龄为245~218 Ma，其滑动方向受控于郯庐断裂带起源期的左行走滑运动。这一系列构造与年代学信息，表明郯庐断裂带起源于华北克拉通与扬子板块的汇聚过程中，代表了这两个大陆的斜向汇聚边界。该断裂带起源期的活动时限，与大别、苏鲁造山带内大陆深俯冲时间相吻合。在大别造山带北部的华北克拉通，原始应存在着向南的突出体(嵌入体)，从而导致嵌入式碰撞与嵌入体边界的大陆斜向汇聚(起源期郯庐断裂带)，符合嵌入式碰撞导致板片撕裂模式。 相似文献
4.
郯庐断裂带形成演化的年代学研究 总被引：11，自引：0，他引：11
通过对郯庐断裂带东侧张八岭蓝片岩带内白云母4 0 Ar - 3 9Ar年龄、断裂带内片麻状花岗岩中钾长石4 0 Ar- 3 9Ar年龄以及断裂带内断层泥K -Ar、ESR年龄的测定 ,并结合有关的地质和古地磁资料 ,厘定了郯庐断裂带形成和演化的过程 :(1)三叠纪 (2 44～ 2 0 9Ma)由于华北与扬子地块碰撞 ,郯庐断裂带形成为其主要左行平移时期 ;(2 )侏罗纪 (189～ 16 4Ma)时郯庐断裂东侧下扬子地块可能经历了逆时针转动 ;(3)白垩纪 (10 3～ 94Ma)开始郯庐断裂带伴随走滑平移而发生正断活动 ;(4)晚白垩—第三纪右旋平移阶段。郯庐断裂的形成与大别 -苏鲁变质带有关。 相似文献
5.
郯庐断裂带南段两侧花岗岩地球化学特征:对大别造山带中-下地壳流动的限定 总被引：1，自引：1，他引：0
大别造山带形成于印支期华南、华北板块陆-陆碰撞过程中。大别造山带造山后发生了山根减薄,其可能的动力学机制为岩石圈拆沉或中-下地壳的塑性流动。为了检验大别造山带是否在造山后发生过中-下地壳流动,本次工作从对比郯庐断裂带南段两侧大别造山带及洪镇、月山地区花岗岩地球化学特征入手,对同样位于郯庐断裂带南段东侧的徐桥岩体开展地球化学研究,为大别造山带造山后是否经历过中-下地壳流动提供证据。本次工作对徐桥岩体的研究表明,该岩体侵位时间为127Ma左右;具有较高的Si O_2和全碱含量;明显富集Rb、Th、U、Pb等大离子亲石元素(LILE),亏损Nb、Ta、Ti等高场强元素(HFSE);稀土元素配分图解中表现为轻稀土富集和重稀土亏损的右倾配分模式,具有较弱的Eu负异常。徐桥岩体的地球化学特征与造山带东侧的月山岩体类似,且与下扬子地区沿江地区侵入岩基本一致。但同样位于造山带东侧的洪镇岩体,其地球化学特征与月山、徐桥岩体明显不同,而与大别造山带一致的地球化学特征,说明两者可能具有相似的源区。基于以上分析,笔者推断洪镇花岗岩的物质来源可能为大别造山带加厚的地壳。而大别造山带东侧出现造山带地壳物质的现象表明造山带在造山后发生过地壳的塑形流动。由于大别造山带中-下地壳物质穿过郯庐断裂带南段,表明郯庐断裂带造山后大规模左行平移事件应发生于大别造山带地壳流动变形之前。 相似文献
6.
徐州利国早白垩世高镁埃达克质侵入岩的成因及其动力学、成矿意义 总被引：2，自引：0，他引：2
位于华北克拉通东南缘、郯庐断裂带西侧的利国岩体形成于白垩纪,由闪长玢岩及少量花岗闪长斑岩组成.与之伴生有一些铜-铁矿化.利国岩体的元素地球化学特征与埃达克岩的地球化学特征非常类似如,SiO2＞56%,较高Al2O3(13.69%～15.15%)、Sr(452×106～617×106)、Sr/Y(30～93)与La/Yb(8～24),但低Y(4.84×106～15.55×106).Vb(0.48×106～1.45×106),无明显的Eu异常(δEu=0.87～0.98).另外,根据其Mg4/5、FeOT/MgO值,又可以分为高锾、较高镁和低镁三类岩石.高镁的岩石类似于赞岐岩.利国埃达克质岩的(87Sr/86Sr)I=0.7055～0.7071,εNd(t)=-11.46～-4.64.不同于俯冲洋壳熔融形成的埃达克岩.我们认为,利国较高镁和低镁埃达克质岩的形成可能与拆沉榴辉质下地壳熔融产生的熔体受到地幔橄榄岩不同程度的混染有关,但是高镁埃达克质岩可能由被拆沉下地壳熔融产生的熔体交代的地幔橄榄岩熔融形成.利国岩体可能是中国东部中生代岩石圈减薄的产物,并可能与郯庐断裂带的活动有关.拆沉榴辉质下地壳熔融产生的熔体与地幔橄榄岩的强烈相互作用可能导致地幔中金属硫化物的分解,并最终导致区内铜矿化. 相似文献
7.
郯庐断裂带庐江段长岗岩体主要由正长花岗斑岩组成。锆石U-Pb定年获得的~(206)Pb/~(238)U加权平均年龄为120±2Ma。样品富集轻稀土元素和大离子亲石元素(如Th、U、K、Pb),亏损重稀土元素和高场强元素(如Nb、Ta、Ti),并具有A型花岗岩的典型特征,如高Fe OT/Mg O、K_2O/Na_2O比值和高的稀土、Zr、Nb含量。长岗A型花岗岩的Sr/Y、La/Yb和Eu/Eu*明显低于郯庐南段埃达克岩,这表明A型花岗岩和郯庐南段埃达克岩岩浆起源深度存在明显差异。A型花岗岩具有高的锆石Ti温度(748~811℃)和低的锆石Ce~(4+)/Ce~(3+)值,这与郯庐南段埃达克岩相一致,暗示A型花岗岩岩浆具有高温和低氧逸度。A型花岗岩具有富集的Sr-Nd同位素组成,类似于大别造山带早白垩世低镁埃达克岩和正常花岗岩,不同于郯庐南段埃达克岩。A型花岗岩锆石δ~(18)O值变化于5.72‰~6.24‰,其ε_(Hf)(t)值(-19.5~-16.9)高于郯庐南段埃达克岩和北大别低镁埃达克岩。本文认为长岗A型花岗岩源自扬子克拉通古元古代中下地壳(t_(DM2)(Hf)=2417~2248Ma),在斜长石稳定且无石榴子石区域(40km)部分熔融形成的。在120Ma之前,作为郯庐南段埃达克岩主要源区的含石榴子石的中-新太古代加厚下地壳(40~50km)已经移除。 相似文献
8.
鸭绿江断裂带的主要特征及其研究意义 总被引：2，自引：0，他引：2
鸭绿江断裂带是郯庐断裂带东侧的一个次级断裂,也是辽宁东部规模较大的断裂带,具有多期活动特点,先后经历了晚印支-早燕山期(T3-J1)左行平移韧性剪切活动、中燕山期(J2-3)早期低角度伸展滑脱和晚期挤压逆冲活动、晚燕山期(K1)至末燕山期(K2)左行正走滑活动、末燕山晚期-喜马拉雅早期(N)右行走滑活动等4个阶段.它控制着侏罗纪、白垩纪岩浆岩、沉积盆地和矿产的分布,也控制着白垩纪中酸性、中基性火山岩喷发.该断裂带为切割地壳硅镁层的深断裂.最大左行平移20 km,最大垂直断距4 km.该断裂带两侧地质构造特征可以对比,对其研究具有重要的指导意义. 相似文献
9.
大别山超高压变质带层析地震调查 总被引：5，自引：0，他引：5
１９９７年３月中德合作进行了大别山科学钻探选址区层析地震调查,研究结果揭示出大别山超高压变质带（ＵＨＰ）地壳精细结构。郯庐断裂带近垂直延伸至Ｍｏｈｏ界面（可能更深）,在Ｍｏｈｏ界面以上郯庐断裂带西侧大别山地壳物质没有迁移进入其东侧。在主测线（横中至潜山镇）２０ｋｍ深度发现一个由西向东倾斜的强反射层,推测可能是一个大的滑脱层。超高压变质岩石（或地幔物质）可能由地幔深处通过郯庐断裂带再沿此滑脱层析返到 相似文献
10.
长期以来对西以郯—庐断裂带为界,东以嘉山—淮阴—响水断裂为界,江苏北部淮(阴)—海(州)变质岩区的构造性质有各种不同的认识。本文从大范围区域重、磁场特征分析,探讨了这一地区郯庐断裂带两侧的构造性质及其成因上的联系,并得出以下的认识:①淮海变质岩区为一多重推覆构造区;②郯庐带西侧的弧形构造为一重力滑推与推覆构造,其成因与郯庐带东侧属华北地台的下元古—元古界变质岩,和其上部沉积盖层成为扬子地台上部的推覆体及其构造发展有直接原因;③扬子地台北向推进及改变推进方向是两侧构造成生、发展的主要原因;④扬子与华北两大地台间在西部郯庐带与北部苏鲁交界附近只有碰接,而不存在 相似文献
11.
Research on the characteristics and influencing factors of terrestrial heat flow in Guizhou Province 
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下载免费PDF全文 Wei Shuai-chao Liu Feng Zhang Wei Wang Gui-ling Yuan Ruo-xi Liao Yu-zhong Yan Xiao-xue 《地下水科学与工程》2022,10(2):166-183
Terrestrial heat flow is an important physical parameter in the study of heat transfer and thermal structure of the earth and it has great significance in the genesis and development and utilization potential of regional geothermal resources. Although several breakthroughs in geothermal exploration have been made in Guizhou Province. The terrestrial heat flow in this area has not been properly measured, restricting the development of geothermal resources in the province. For this reason, the terrestrial heat flow in Guizhou was measured in this study, during which the characteristics of heat flow were determined using borehole thermometry, geothermal monitoring and thermal property testing. Moreover, the influencing factors of the terrestrial heat flow were analyzed. The results show that the thermal conductivity of rocks ranges from 2.0 W/(m·K) to 5.0 W/(m·K), with an average of 3.399 W/(m·K); the heat flow varies from 30.27 mW/m2 to 157.55 mW/m2, with an average of 65.26 ± 20.93 mW/m2, which is slightly higher than that of the average heat flow in entire land area in China. The heat flow in Guizhou generally follows a dumbbell-shaped distribution, with high values present in the east and west and low values occurring in the north and south. The terrestrial heat flow is related to the burial depths of the Moho and Curie surface. The basaltic eruptions in the Emeishan led to a thinner lithosphere, thicker crust and lateral emplacement, which dominated the basic pattern of heat flow distribution in Guizhou. In addition, the dichotomous structure of regional active faults and concealed deep faults jointly control the heat transfer channels and thus influence the terrestrial heat flow. 相似文献
12.
Temperature measurements carried out on 9 hydrocarbon exploration boreholes together with Bottom Simulating Reflectors (BSRs) from reflection seismic images are used in this study to derive geothermal gradients and heat flows in the northern margin of the South China Sea near Taiwan. The method of Horner plot is applied to obtain true formation temperatures from measured borehole temperatures, which are disturbed by drilling processes. Sub-seafloor depths of BSRs are used to calculate sub-bottom temperatures using theoretical pressure/temperature phase boundary that marks the base of gas hydrate stability zone. Our results show that the geothermal gradients and heat flows in the study area range from 28 to 128 °C/km and 40 to 159 mW/m2, respectively. There is a marked difference in geothermal gradients and heat flow beneath the shelf and slope regions. It is cooler beneath the shelf with an average geothermal gradient of 34.5 °C/km, and 62.7 mW/m2 heat flow. The continental slope shows a higher average geothermal gradient of 56.4 °C/km, and 70.9 mW/m2 heat flow. Lower heat flow on the shelf is most likely caused by thicker sediments that have accumulated there compared to the sediment thickness beneath the slope. In addition, the continental crust is highly extended beneath the continental slope, yielding higher heat flow in this region. A half graben exists beneath the continental slope with a north-dipping graben-bounding fault. A high heat-flow anomaly coincides at the location of this graben-bounding fault at the Jiulong Ridge, indicating vigorous vertical fluid convection which may take place along this fault. 相似文献
13.
天然气水合物广泛分布于海底和永久冻土带。自20世纪末以来,新西兰北岛东坡希古朗基陆架和澳大利亚新喀里多尼亚盆地相继被科学家发现了天然气水合物标志BSR(BottomSimulatingReflector),这引起世界广泛关注,文章结合以前的研究工作,从地热角度剖析天然气水合物赋藏状况。依据国际热流委员会(IHFC)提供的西南太平洋地热数据,经过统计确定出该区域的热流分布;计算得出该区域热流平均值为80.1mW/m2,低于全球大洋边缘盆地地区平均热流值101±2.2mW/m2;结合天然气水合物温压方程,计算结果表明西南太平洋天然气水合物稳定带厚度平均值为274±20m,薄于其他已经发现的海洋天然气水合物稳定带平均厚度(约400m)。文章还定量分析了温度参数对天然气水合物稳定带的影响。 相似文献
14.
Eleven new estimates of heat flow (q) from the southern Altai-Sayan Folded Area (ASFA) have provided update to the heat flow map of Gorny Altai. Measured heat flow in the area varies from 33 to 90 mW/m2, with abnormal values of >70 mW/mq at four sites. The anomalies may have a deep source only at the Aryskan site in the East Sayan (q = 77 mW/m2) while high heat flows of 75–90 mW/m2 obtained for the Mesozoic Belokurikha and Kalguty plutons appear rather to result from high radiogenic heat production in granite, which adds a 25–30 W/m2 radiogenic component to a deep component of 50–60 mW/m2. The latter value is consistent with heat flow estimates derived from helium isotope ratios (54 mW/m2 in both plutons). Heat flow variations at other sites are in the range from 33 to 60 mW/m2. The new data support the earlier inferences of a generally low heat flow over most of ASFA (average of 45–50 mW/m2) and of a “cold” Cenozoic orogeny in the area (except for southeastern ASFA), possibly driven by shear stresses associated with India indentation into Eurasia. 相似文献
15.
江汉盆地当阳复向斜当深3井实测地温剖面和样品热导率测试结果表明:其现今地温梯度为20～24℃/km,热流值为56mW/m2,体现了盆地发育于扬子稳定陆块的大地构造属性。基于7个磷灰石裂变径迹样品和大量镜质体反射率古温标数据进行的热史恢复表明,盆地构造—热演化经历了前印支期的低热流(50～60mW/m2)和小剥蚀量(50～200m),印支期的高热流(约80mW/m2)及燕山期与喜马拉雅期的低热流(50～60mW/m2)与大剥蚀量(1100～2400m)的不同演化阶段,反映了盆地和区域构造演化过程的阶段性。受沉积剥蚀及盆地构造—热演化的控制,生油岩系的生烃阶段与过程具有多期次的特征。 相似文献
16.
The GALO system is applied to the numerical reconstruction of burial and thermal histories of the West Bashkirian lithosphere from the Riphean to the present. An analysis of the variation in tectonic subsidence of the basin during its development is utilized to estimate approximately the mantle heat flow variations. Our variant of basin evolution suggests that after cooling in the Early Riphean, the rather weak thermal reactivations have not led to considerable heating of the lithosphere in the study region. Surface heat flow decreased from relatively high values in the Early Riphean (60–70 mW/m2 in the eastern area and 40–50 mW/m2 in the western part) to present-day values of 32–40 mW/m2. In spite of the relatively low temperature regime of the basin as a whole, a syn-rifting deposition of more than 10 km of limestone, shale and sandstone in the Riphean resulted in rather high temperatures (180–190 °C) at the base of present-day sedimentary blanket in the eastern area. In agreement with the observed data, computed present-day heat flow through the sediment surface increases slightly from 32 to 34 mW/m2 near the west boundary of the region to 42 mW/m2 near the boundary of the Ural Foldbelt, whereas the heat flow through the basement surface decreases slightly from 28–32 to 24–26 mW/m2 in the same direction. The mantle heat flow is only 11.3–12.7 mW/m2, which is considerable lower than mean heat flow of the Russian Platform (16–18 mW/m2) and comparable with the low heat flow of Precambrian shields. 相似文献
17.
仲巴裂谷位于藏南裂谷系的西侧,其断层发育、断错地貌清晰. 但目前,该断裂活动性研究尚属空白,制约了对整个藏南裂谷系变形机制的探索.基于GIS空间分析技术,利用数字高程模型数据系统提取该区的河流地貌参数,包括地形坡度、地形起伏度、河流陡峭指数和裂点等. 对该裂谷两侧36个流域盆地的地形参数结果进行统计和分析后发现:地形坡度与ksn之间具有一致性,仲巴裂谷西侧北、中段坡度陡峭,ksn值较高,南段支流中间部分陡峭,两端较缓,对应ksn值中间高两端低;东侧坡度和ksn分布呈现中段陡峭,两端变缓的特征. 河流纵剖面上表现出裂点上下陡峭系数的差异,东西两侧河流均在出水口处河段有最高河道陡峭系数,向上游段减小,总体上西侧河道陡峭系数大于东侧. 综合地形坡度、河流纵剖面及裂点分析结果,认为仲巴裂谷西侧断裂的构造活动性可能强于东侧. 相似文献
18.
Makoto Yamano Masataka Kinoshita Shusaku Goto 《International Journal of Earth Sciences》2008,97(2):345-352
Thirty-three new measurements on the seaward slope and outer rise of the Japan Trench along a parallel of 38°45′N revealed
the existence of high heat flow anomalies on the subducting Pacific plate, where the seafloor age is about 135 m.y.. The most
prominent anomaly with the highest value of 114 mW/m2 is associated with a small mound on the outer rise, which was reported to be a kind of mud volcano. On the seaward slope
of the trench, heat flow is variable: high (70–90 mW/m2) at some locations and normal for the seafloor age (about 50 mW/m2) at others. The spatial variation of heat flow may be related to development of normal faults and horst/graben structures
due to bending of the Pacific plate before subduction, with fluid flow along the fault zones enhancing the vertical heat transfer.
Possible heat sources of the high heat flow anomalies are intra-plate volcanism in the last several million years like that
discovered recently on the Pacific plate east of the Japan Trench. 相似文献
19.
2-D Crustal thermal structure along Thuadara-Sindad DSS profile across Narmada-Son lineament,central India 总被引：1，自引：0，他引：1
Central India is traversed by a WSW-ENE trending Narmada-Son lineament (NSL) which is characterized by the presence of numerous
hot springs, feeder dykes for Deccan Traps and seismicity all along its length. It is divided in two parts by the Barwani-Sukta
Fault (BSF). To the west of this fault a graben exists, whereas to the east the basement is uplifted between Narmada North
Fault (NNF) and Narmada South Fault (NSF). The present work deals with the 2-D thermal modeling to delineate the crustal thermal
structure of the western part of NSL region along the Thuadara-Sindad Deep Seismic Sounding (DSS) profile which runs almost
in the N-S direction across the NSL. Numerical results of the model reveal that the conductive surface heat flow value in
the region under consideration varies between 45 and 47mW/m2. Out of which 23mW/m2 is the contribution from the mantle heat flow and the remaining from within the crust. The Curie depth is found to vary between
46 and 47 km and is in close agreement with the earlier reported Curie depth estimated from the analysis of MAGSAT data. The
Moho temperature varies between 470 and 500°C. This study suggests that this western part of central Indian region is characterized
by low mantle heat flow which in turn makes the lower crust brittle and amenable to the occurrence of deep focused earthquakes
such as Satpura (1938) earthquake. 相似文献
20.
The Dniepr–Donets Basin (DDB) is a Late Devonian rift structure located within the East-European Craton. Numerical heat flow models for 13 wells calibrated with new maturity data were used to evaluate temporal and lateral heat flow variations in the northwestern part of the basin.The numerical models suggest that heat flow was relatively high during Late Carboniferous and/or Permian times. The relatively high heat flow is probably related to an Early Permian re-activation of tectonic activity. Reconstructed Early Permian heat flow values along the axial zone of the rift are about 60 mW/m2 and increase to 90 mW/m2 along the northern basin margin. These values are higher than those expected from tectonic models considering a single Late Devonian rifting phase. The calibration data are not sensitive to variations in the Devonian/Carboniferous heat flow. Therefore, the models do not allow deciding whether heat flows remained high after the Devonian rifting, or whether the reconstructed Permian heat flows represent a separate heating event.Analysis of the vitrinite reflectance data suggest that the northeastern Dniepr–Donets Basin is characterised by a low Mesozoic heat flow (30–35 mW/m2), whereas the present-day heat flow is about 45 mW/m2. 相似文献