共查询到19条相似文献，搜索用时 161 毫秒
1.
深部温度场与岩石圈热结构特征是认识地热系统深部热源机理的重要途径。本文在系统分析渭河盆地及其邻区现今大地热流特征基础上,基于旬邑—西峡宽角反射/折射地震测深剖面揭示的地壳分层结构,采用二维有限元方法,对渭北隆起、渭河盆地以及北秦岭构造带的深部温度场和岩石圈热结构开展数值模拟研究,在此基础上分析渭河盆地地热系统深部热源机理。结果表明,旬邑—西峡剖面上大地热流介于57.6～75.7mW/m2之间,平均为(70.4±4.7)mW/m2;地幔热流在29.5～38.6mW/m2之间,平均值为34.1mW/m2;莫霍面温度变化范围约在600～740℃之间;“热”岩石圈厚度约为95～110km。从渭北隆起—渭河盆地—秦岭造山带,大地热流、莫霍面温度和地幔热流值表现出低→高→低的变化规律,相应地“热”岩石圈厚度则表现出厚→薄→厚的变化趋势。渭河盆地地壳厚度减薄明显,莫霍面温度显著高于渭北隆起和秦岭造山带,暗示着渭河盆地地壳活动性显著。然而,从渭北隆起—渭河盆地—秦岭造山带,“热”岩石圈厚度变化范围不大,且渭河盆地内... 相似文献
2.
英雄岭构造带是柴达木盆地油气最为富集的地区之一,地温场对油气成藏过程有重要影响,也是油田开发工程实施的重要参考.利用试油静温数据,结合激光扫描法开展岩心热导率及放射性生热测试,对研究区地温场进行了研究.英东地区地温梯度为31.8～35.3℃/km,平均为33.6℃/km,新近系热导率为1.8～2.4W/m/K,平均为2.07W/m/K,大地热流值为65～74mW/m2,平均为69mW/m2.热流呈“西高东低”特征,昆北、南翼山及一里坪等地热流值超过65mW/m2,而阿尔金山前、冷湖构造带及涩北等地较低,咸水泉和冷湖等地普遍低于50mW/m2.新近系实测平均生热率为2.84μW/m3,对热流的贡献约20%.研究区具有“热壳温幔”特征,其影响因素包括地壳放射性生热、蚀源区高U中酸性侵入岩、印度板块汇聚引起的构造热及热岩石圈厚度较薄等. 相似文献
3.
现今地温场是构造活动、岩石圈热状态的综合反应,对研究盆地的区域构造演化、深部岩石圈结构和评估油气潜力具有重要意义。地温梯度和大地热流是表征沉积盆地热状况的两个基本参数。虽然我国大陆地区地热数据较丰富,并已经过四次系统汇编,但中国海及邻区盆地地热数据报道较少,且未经过系统整理。本文基于近年来新增的钻井温度数据,新增计算研究区810个地温梯度数据,并收集了国内外数据库、期刊的地热数据,在此基础上,首次系统整理了中国海及邻区盆地地温梯度数据和大地热流数据,绘制了其等值线图,分析了研究区现今地温场特征并讨论了其影响因素。研究结果表明,中国海及邻区盆地平均地温梯度43.2±25.7℃/km,平均大地热流74.4±26.6 mW/m2,多数盆地平均大地热流高于65 mW/m2,属于“热盆”;地温场分布总体呈现较为明显的“两带性”,其中近岸带较冷,远岸带较热;研究区现今地温场特征直接或间接地受控于其所处的构造环境,整体上是太平洋板块等多板块作用下岩石圈伸展减薄的结果,局部地区的热异常可能与断裂活动、岩浆活动、泥-热流底辟活动等因素有关。 相似文献
4.
阿留申俯冲带位于环太平洋俯冲带最北端,是东太平洋型俯冲和西太平洋俯冲的过渡区域。该俯冲带火山岛弧距离海沟的距离从东向西逐渐增大,而形成地球上独特的岛弧火山链与海沟V字型斜交的现象。这一现象的运动学成因目前并没有统一的认识。本文通过对阿留申俯冲带几何形态数据、运动学数据进行整理分析,尝试运用构造赤道理论探讨该现象形成的运动学背景。阿留申俯冲带的几何学数据表明:从俯冲带东段(175°E)至俯冲带西段(155°W),火山岛弧距俯冲海沟的距离从80 km增加至250 km。与此同时,俯冲板片的倾角由60°减小至30°。板块的运动学分析表明:相对北美板块,太平洋板块的东段的运动矢量为48 mm/a,向北运动;逐渐转变为西段的78mm/a,向西北方向运动。相对于软流圈,太平洋板块的运动方向没有改变,始终向西北方向运动,速率向西逐渐增加。因此,在俯冲带的东段太平洋板块的绝对运动方向和相对运动方向存在30°左右的夹角,而这个夹角在西段几乎不存在。太平洋板块的绝对运动方向和相对运动方向之间的夹角不同,会导致软流圈对俯冲板片的反作用力差异,从而形成不同的俯冲角度和俯冲带宽度。太平洋板块相对北美板块和相对地幔的速度方向夹角的变化被认为是引起阿留申火山弧与海沟"V"字型斜交的运动学成因。 相似文献
5.
6.
在大地热流密度分布的基础上,本文基于二维稳态热传导方程,根据研究区热导率、生热率等热物理性质参数,对横穿川东北地区、秭归盆地、黄陵穹窿和江汉盆地等几个构造单元的奉节（FJ）-观音垱（GYD）地学剖面进行了温度场数值模拟研究,获得了其深部热结构认识。模拟结果显示,地幔热流自西向东逐渐升高,变化范围约为25.3～34.7 mW/m2。莫霍面温度大约在380 ℃～450 ℃之间变化。热岩石圈厚度自西向东先稍微增厚,后逐渐变薄,变化范围约为115～171 km。江汉盆地中新生代的伸展作用使其地幔热流稍有升高,“热”岩石圈厚度相对较薄（约116 km）,而川东北地区则受到早期的挤压和晚期的抬升剥蚀作用,地幔热流相对较低,其深部“热”岩石圈厚度也相对较厚（约168 km）。 相似文献
7.
8.
根据近年来全球地壳上地幔探测的成果,分析了洋陆转换、地壳和岩石圈加厚的作用过程。洋陆转换作用可分为以下五个演化阶段：① 同大洋扩张期的地壳增厚;② 海沟发生与早期俯冲;③ 俯冲带成熟与沟弧盆体系形成;④ 俯冲带汇聚和位移;⑤ 陆—岛碰撞和陆壳连接。同大洋扩张期的地壳增厚作用指发生在被动大陆边缘的地质作用。包括沉积作用,岩浆底侵作用,下地壳和岩石圈地幔压裂,形成海沟等。海沟形成后陆缘转变为主动大陆边缘,大地构造机制转换为板块俯冲作用。成熟期的洋—陆转换作用特征是海盆扩张和板块俯冲造成的洋壳缩短取得平衡。弧后盆地和弧后边缘海的打开,表明俯冲带进入完全成熟的阶段。洋脊俯冲之后过成熟期的洋—陆转换作用,其特征是海盆逐渐缩小而且板块俯冲带汇聚。这里既有密集的俯冲带又有短期打开的边缘海岭;俯冲带不断位移,既可后撤也可前冲;俯冲板块经常发生断裂和拆沉。过成熟期的板块俯冲结果是边缘海微板块的萎缩。经过陆—岛碰撞,岛弧地壳增厚,与大陆板块连为一体,成为大陆内部的一个构造单元,即显生宙的“古洋—陆转换带”。 相似文献
9.
依据236口井共2 706组的静温数据以及25口井的系统测温数据,分析计算了渤海盆地地温梯度及大地热流;建立地壳分层结构模型,利用回剥法计算现今地幔热流、深部温度以及岩石圈厚度;在此基础上,利用地球动力学方法恢复本区热流演化史。结果表明：渤海盆地背景地温梯度为322 ℃/km,热流值为648 mW/m2;盆地现今热岩石圈厚度在61~69 km之间,地幔热流占地表热流的比例在60%左右,属于“热幔冷壳”型岩石圈热结构,盆地地壳底部或莫霍面温度变动在548~749 ℃之间;热流演化的特征与盆地的构造演化背景吻合,新生代以来盆地经历了3期岩石圈减薄并加热的过程,在东营组沉积末期热流达到最高(70~83 mW/m2）,这期间盆地内产出多期碱性玄武岩,表明盆地经历了波及地幔的裂谷过程,随后进入热沉降期,热流逐渐降低,盆地向坳陷型转变。 相似文献
10.
大陆克拉通是地球表面上相对稳定的构造单元。从地热学的角度考虑,克拉通岩石圈的稳定意味着地表热流等于对流地幔岩石圈底部提供的热流加上岩石圈内部由放射性衰变产生的热量。太古代稳定克拉通一般具有冷的地热特征,且处于热平衡状态。打破克拉通热平衡的因素有多种,如岩石圈地幔的放射性生热、来自深部的地幔柱、板块俯冲等。华北是全球古老克拉通遭受破坏最明显和最典型的地区,其破坏与中生代太平洋板块向东亚的深俯冲密切相关。古太平洋板块快速俯冲并停滞在地幔转换带脱水、形成宽约1 000 km的低粘大地幔楔,导致地幔对流增强。在活跃地幔对流的热侵蚀与橄榄岩-熔体相互作用共同作用下,华北克拉通在中生代期间迅速减薄。经过中生代加热减薄的华北克拉通岩石圈强度显著变弱,在俯冲板块后撤作用下,岩石圈拉张并进一步减薄,地表热流升高。华北克拉通破坏是一个漫长的历程,期间大地热流的演化特征呈现出由中生代以前的低值演化至新生代的高值再过渡到现今的中等状态（接近全球大陆平均值）。 相似文献
11.
ABSTRACT Active and remnant back-arc regions do not follow a typical conductive lithosphere cooling model, but instead have an apparent two-stage cooling, defined by a high heat flow back-arc region during subduction and a second post-subduction heating event that extends elevated heat flow for several 10s million years. Numerical one-stage cooling models have not reproduced observed heat flow anomalies in active subduction zones using physically realistic parameters and require a secondary post-subduction heating mechanism. Here, an extension driven-volcanism model is developed to examine extension driven heating and volcanism as a mechanism to produce a prolonged thermal anomaly within back-arc lithosphere. This model is tested using the recorded thermal evolution of the Northern Cordillera Volcanic Province (NCVP), a Neogene-Quaternary alkaline volcanic province located in the remnant back-arc region of the Pacific-North American subduction zone in British Columbia, Canada. A single steady-state lithosphere geotherm does not intersect all previously published temperature estimates, suggesting previous data record the thermal evolution of the NCVP. Calculated geotherms at equilibrium with the minimum and maximum MELTS temperatures predict an increase in reduced mantle heat flow (Qm ) from 43 to 72 mW/m2 and lithosphere thinning from a depth of 87 to 48 km. The newly developed extension-volcanism model reproduced the calculated pre- and post-volcanism thermal regimes for the NCVP and supports that extension within the remnant back-arc could produce the present heat flow anomaly and volcanism. The model most readily produces volcanism when Qm is ~45–65 mW/m2, a typical range for back-arcs. Back-arc regions are prime locations for limited volcanism because their warmer thermal regime minimizes tectonic stress requirements to produce volcanism. Additionally, two-stage cooling of back-arcs can be explained with a time-dependent extension-volcanism thermal feedback mechanism that is possible because of the subduction driven pre-heating of back-arc regions. 相似文献
12.
The asthenosphere upwelled on a large scale in the western Pacific and South China Sea during the Cenozoic,which formed strong upward throughflow and caused the thermal structure to be changed obviously.The mathematical analysis has demonstrated that the upward throughflow velocity may have varied from 3×1011 to 6×1012 m/s.From the relationship between the lithospheric thickness and the conductive heat flux,the Hthospherie heat flux in the western Pacific should be above 30 mW/m2,which is consistent with the observed data.The huge low-speed zone within the upper mantle of the marginal sea in the western Pacific reflects that the upper mantle melts partially,flows regionally in the regional stress field,forms the upward heat flux at its bottom,and causes the change of the lithospheric thermal structure in the region.The numerical simulation result of the expansion and evolution in the South China Sea has demonstrated that in the early expansion,the upward throughflow velocity was relatively fast,and the effect that it had on the thickness of the lithosphere was relatively great,resulting in the mid-ocean basin expanding rapidly.After the formation of the ocean basin in the South China Sea,the upward throughflow velocity decreased,but the conductive heat flux was relatively high,which is close to the actual situation.Therefore,from the heat transfer point of view,this article discusses how the upward heat flux affects the lithospheric thermal structure in the western Pacific and South China Sea.The conclusions show that the upward heat throughflow at the bottom of the llthospheric mantle resulted in the tectonic deformation at the shallow crust.The intensive uplifts and rifts at the crust led to the continent cracks and the expansion in the South China Sea. 相似文献
13.
西太平洋区域是全球地质构造和海陆相互作用最活动的区域,经过50多年的大洋钻探研究,人们对西太平洋弧后海底扩张成因、俯冲工厂的动力学机制、地幔演化过程、发震带、热点岩浆活动、沉积古环境等都有了深入研究和分析,但是西太平洋边缘海盆具有很大的构造多样性和复杂性,仍然有很多的科学目标和科学问题有待进一步开展研究.本文详细分析了边缘海盆的大洋岩石圈演化特殊性,原位上地幔蛇纹岩化的程度,初始俯冲与初始扩张的形成机制,海台、海山、海岭、洋脊、洋隆的属性,洋中脊水热循环活动的强度及其对大洋岩石圈演化的影响,岩石圈共轭张裂与破裂模式与机制,大洋红层与异常沉积这7个方面的科学问题,并建议就流体地球化学剖面、海山岩浆剖面、穆绍海沟与加瓜海脊、Ayu海槽、卡罗琳海岭系统、Eauripik海岭、冲绳海槽、莫霍面这8个关键具体目标开展详细的地球物理刻画并提出具有全球意义的钻探建议,为今后实现中国领导的全球大洋钻探工作提供思路. 相似文献
14.
The region under study is located in the active “transition zone” from the Eurasian continent to the Pacific Ocean. The zone occupies not only the continent-ocean border area (continental coastline, marginal seas, island arcs, and deep-sea trenches) but also the margins of intracontinental regions of the Eurasian continent with different structures and regimes of development. The transition zone is a natural buffering and damping regulator of the interaction between the Eurasian and Pacific plates and is characterized by intense orogenesis, contemporary volcanism, active seismicity, diverse geothermal regime, and highly nonuniform measured heat-flow values. Available geothermal data for the region are not sufficiently generalized. After the latest maps compiled in the 1990s, new data have been obtained and new geoinformation technologies have been developed. In the study presented in this paper, available geothermal information has been generalized and a detailed heat flow distribution map has been compiled and used to calculate Moho temperatures, to determine the thickness of the “geothermal” lithosphere, and to construct distribution maps of these parameters. 相似文献
15.
A secondary flow model for back-arc spreading is developed in this paper that shows some of the characteristics of observed back-arc spreading. Back-arc spreading has formed marginal seas around the west and southwest rim of the Pacific. The episodic spreading and different directions of opening are not completely understood; however, there does appear to be a limited lifetime (< 17 m.y.) and when one episode of spreading ends, there is a lag time (6–10 m.y.) before another adjacent one begins. This suggests that back-arc flow is caused by secondary flow induced by subduction. Simple scaling arguments with physically reasonable values suggest that forced and free convection effects will be nearly equal. A two-dimensional, finite difference model is developed and several numerical experiments lasting 160 m.y. with a varying subduction rate are discussed. These experiments show stress surges lasting 10–20 m.y. and a series of eddies and counter-eddies behind the trench with a spatial scale of 300–400 km. This supports the idea that back-arc spreading is the result of transient eddies induced by the subducting slab. 相似文献
16.
The lithospheric sinking along subduction zones is part of the mantle convection. Therefore, computing the volume of lithosphere recycled within the mantle by subducting slabs quantifies the equivalent amount of mantle that should be displaced, for the mass conservation criterion. The rate of subduction is constrained by the convergence rate between upper and lower plates and the motion of the subduction hinge H that may either converge or diverge relative to the upper plate. Here, starting from the analysis of the slab hinge kinematics, we evaluate the subduction rate at 31 subduction zones worldwide, useful to compute volumes of sinking lithosphere into the mantle. Our results show that ∼190 km3/yr and ∼88 km3/yr of lithospheric slabs are currently subducting below H-divergent and H-convergent subduction zones, respectively. We also propose supporting numerical models providing asymmetric volumes of the subducted lithosphere, using the subduction rate instead of plate convergence, as boundary condition. Furthermore, H-divergent subduction zones appear to be coincident with subductions having “westward”-directed slabs, whereas H-convergent subduction zones are mostly compatible with those that have “eastward-to-northeastward”-directed slabs. On the basis of this geographical polarity, our lithospheric volume estimation gives ∼214 km3/yr and ∼88 km3/yr of subducting lithosphere, respectively. This entails that W-directed subduction zones contribute more than twice in lithospheric sinking into the mantle with respect to E-to-NE-directed ones. In accordance with the conservation of mass principle, this volumetric asymmetry in the mantle suggests a displacement of ∼120 km3/yr of mantle material from west to east, providing a constraint for global asymmetric mantle convection. 相似文献
17.
The shapes and orientations of Benioff zones beneath island arcs, interpreted as marking the location of subducted lithosphere, provide the best presently available constraints on the global convective flow pattern associated with plate motions. This global flow influences the dynamics of subduction. Subduction zone phenomena therefore provide powerful tests for models of mantle flow. We compute global flow models which, while simple, include those features which are best constrained, namely the observed plate velocities, applied as boundary conditions, and the density contrasts given by thermal models of the lithosphere and subducted slabs. Two viscosity structures are used; for one, flow is confined to the upper mantle, while for the other, flow extends throughout the mantle.Instantaneous flow velocity vectors match observed Benioff zone dips and shapes for the model which allows mantle-wide flow but not for the upper mantle model, which has a highly contorted flow pattern. The effect of trench migration on particle trajectories is calculated; it is not important if subduction velocities are greater than migration rates. Two-dimensional finite element models show that including a coherent high viscosity slab does not change these conclusions. A coherent high viscosity slab extending deep into the upper mantle would significantly slow subduction if flow were confined to the upper mantle. The maximum earthquake magnitude, Mw, for island arcs correlates well with the age of the subducted slab and pressure gradient between the trench and back-arc region for the whole mantle, but not the upper mantle, flow model. The correlations with orientations of Benioff zones and seismic coupling strongly suggest that the global return flow associated with plate motions extends below 700 km. For both models, regions of back-arc spreading have asthenospheric shear pulling the back-arc toward the trench; regions without back-arc spreading have the opposite sense of shear, suggesting global flow strongly influences back-arc spreading. 相似文献
18.
The Blovice accretionary complex, Bohemian Massif, hosts well-preserved basaltic blocks derived from an oceanic plate subducted beneath the northern active margin of Gondwana during late Neoproterozoic to early Cambrian. The major and trace element and Hf–Nd isotope systematics revealed two different suites, tholeiitic and alkaline, whose composition reflects different sources of melts within a back-arc basin setting. The former suite has composition similar to mid-ocean ridge basalts (MORB), yet with striking enrichment in large-ion lithophile elements (LILE) and Pb paralleled by depletion in Nb, in agreement with its derivation from depleted mantle fluxed by subduction-related fluids. In contrast, the latter suite has composition similar to ocean island basalts (OIB) with variable contribution of ancient, recycled crustal material. We argue that both suites represent volcanic members of Ocean Plate Stratigraphy (OPS) and indicate that the oceanic realm consumed by the Cadomian subduction was a complex mosaic of intra-oceanic subduction zones, volcanic island arcs, and back-arc basins with mantle plume impinging the spreading centre. Hence, the basalt geochemistry implies that two distinct domains of oceanic lithosphere may have existed off the Gondwana’s continental edge: an outboard domain, made up of old and less buoyant oceanic lithosphere (remnants of the Mirovoi Ocean surrounding former Rodinia?) that was steeply subducted and generated the back-arcs, and young, hot, and more buoyant oceanic lithosphere generated in the back-arcs and later involved in accretionary complexes as dismembered OPS. Perhaps the best recent analogy of this setting is the Izu Bonin–Mariana arc–Philippine Sea in the western Pacific. 相似文献
19.
Geothermal Characteristics and Geological Implications of Major Tectonic Units in China 总被引：4，自引：0，他引：4
Wang Yang Faculty of Earth Sciences Mineral Resources China University of Geosciences Beijing China Wang Jiyang Institute of Geology Geophysics Chinese Academy of Sciences Beijing China Deng Jinfu Faculty of Earth Scie 《中国地质大学学报(英文版)》2000,11(3)