长江中下游区域地壳热结构及研究意义

统地测制了从基底到盖层两条基干剖面，分析了上地壳不同构造层各岩类Ｕ，Ｔｈ．Ｋ自发裂变产热元素的质量分数，计算出各结构层热流值、各层配分比例及温度分布；对于下地壳，则利用地震波速与热产率、热流和温度分布的相关性进行了估算，从而建立起长江中下游地区地壳热结构模型。长江中下游地壳热流（ｑｃ）为３１．２７－３２．１７ｍＷ·ｍ２，占地表热流的５０．８％～５３．６９％；下地壳在整个地壳热流值中所占比例最小（约３．０％－７．５％）；地幔热流（ｑｍ）约占地表热流的一半     

南海东北陆缘的地壳速度结构及其构造意义:来自广角地震剖面的约束

南海东北部深部地壳结构蕴含着南海陆缘伸展张裂过程的重要信息。在南海东北陆缘布设的一条广角地震测线(DP13)沿NW-SE方向依次穿过东沙隆起和台西南盆地。本文利用射线追踪和正演走时拟合软件RayInvr构建地壳纵波速度结构,模型表明：沉积层速度1.6～4.6 km/s,厚度0.5～3.8 km,横向分布不均匀,沉积基底起伏剧烈;莫霍面埋藏深度由陆架区的25.5 km急剧减小到陆坡下方的13 km,随后向下陆坡远端增深至16 km;陆架处东沙隆起下方地壳厚度从～25 km减薄到～21 km,下陆坡远端地壳厚约10～13 km,地壳拉张因子分别为1.3～1.5和2.6～3.1,表现为轻微和中等减薄;陆坡区台西南盆地内地壳厚度从17 km急剧减薄至7～8 km,地壳拉张因子高达4.6,呈超伸展减薄;地壳厚度由陆向海非单调减薄,地壳伸展具有明显的空间差异性;陆架-上陆坡和下陆坡下地壳底部发现两个相对孤立的不连续高速体,速度分别为7.0～7.5 km/s和7.0～7.3 km/s,厚度分别3～5 km和1～3 km,前者位于古太平洋俯冲带前缘,几乎与南海东北部高磁异常重叠,推测由中生代古太平洋板...     

南海北部陆缘地壳结构特征及其构造过程

根据“北部湾大陆缘地壳结构ＰＳ转换波测深”等地球物理测量结果,本文研究了南海北部陆缘的地壳结构特征,讨论了其白垩纪以来的构造过程。地球物理测量表明,由陆向海,南海北部陆缘地壳由陆壳、过渡壳变为洋壳,厚度由３４ｋｍ减薄至８ｋｍ左右。垂向上地壳为３层结构模式。陆壳、过渡壳和洋壳的下地壳Ｐ波速度普遍较高。地壳伸展系数的计算表明南海北部陆缘伸展主要发育于陆坡地区。结合区域地质研究,本文认为：南海北部陆缘及     

青海共和盆地岩石圈热-流变结构及地热意义

地球深度热状况是深部地球动力学和岩石圈活动性研究的重要内容, 岩石圈热结构和热-流变结构可以很好地揭示岩石圈范围内的热状况。近年来, 在青海共和盆地钻探揭露了深部高温干热岩体, 关于其热源机制尚未有定论。本文以青海共和盆地为研究对象, 分析壳内温度分布和流变强度, 探讨壳内低速体的地质属性。结果表明, 共和盆地的地壳流变结构从上而下分为脆性和韧性两层, 韧性层又包括中地壳和下地壳两层韧性层, 在上地壳尺度均表现为脆性破裂为主, 并逐渐过渡为韧性流变; 恰卜恰地区在脆性破裂的上地壳延伸至中下地壳时, 破裂沿一系列滑脱面发生韧性滑动, 局部地段形成壳内熔融, 为恰卜恰地区提供了额外的热源, 使其大地热流值(109.6 mW/m2)显著高于贵德地区(77.6 mW/m2)。这一认识为共和盆地壳内低速体存在提供了新的佐证, 也为区内干热岩热源分析以及高温地热资源探测开发提供了科学依据。     

张裂陆缘地壳结构特征与张裂模式

张裂陆缘作为威尔逊旋回中关键的一环,是研究地球板块构造及其演化过程的重要构造单元.本文阐述了3种类型张裂陆缘(富岩浆型、贫岩浆型和中间型)的地壳结构特征,总结了它们的演化过程与机制,分析表明构造作用、岩浆活动程度、先存结构等是形成不同类型张裂陆缘的主要控制因素.针对南海北部陆缘复杂的构造属性与演化机制问题,提出了今后重...     

南海华南陆缘中生界层序地层模式与海平面变化

华南陆缘中生界地层以广东省出露最广,这套地层为陆源碎屑沉积岩,局部为火山岩。上三叠统—上白垩统划分为2个巨层序、7个超层序和15个层序。沉积充填序列展示出本地区经历了海侵-海退过程,沉积环境由海相转化为陆相环境。3个级别的海平面变化控制了层序、超层序和巨层序的发育。粤中--粤东地区中生界发育的Ⅲ级层序可归纳出3种类型:浅水型、深水型和湖盆型;浅水型层序又可以分为浅水Ⅰ型和浅水Ⅱ型。     

贵德盆地热结构及地热成因机制

贵德盆地位于青藏高原东北缘黄河谷地之中, 四周环山, 为新生代断陷盆地, 地貌单元位于青藏块体, 地处祁连、昆仑和秦岭三大褶皱系交汇地带; 新构造活动强烈, 发育一系列NWW向、NW向及NNW向断裂, 为区内高温地热系统提供了较好的地热地质条件。区内地热显示类型多样, 水热活动剧烈, 尤其是盆地西部的扎仓寺热田, 水温高达 93℃, 蕴藏着丰富的地热资源。但是由于客观条件限制, 区内地热资源的开发利用及相关研究尚有不足之处。     

华南东部陆缘新生代隆升历史及其动力学机制

华南陆缘在新生代期间经历了千米量级的上覆盖层剥蚀和山脉隆升;同时,其东侧的东海陆架盆地经历多次构造应力场的反转并发育多期反转构造。东海陆架盆地内的构造反转与华南陆缘隆升的发生时间和触发机制是否一致有待研究。为此,本文对浙江地区的岩石样品进行磷灰石裂变径迹测试和热演化史反演分析其隆升历史,并通过地震剖面分析东海陆架盆地的反转时间及其反转所导致的地层剥蚀量;最后,将二者进行对比分析并研究其动力学机制。结果发现,华南东部陆缘地区至少存在晚始新世（34.5~33.5Ma）、中中新世（16~11.5Ma）、上新世以来（5~0Ma）三期明显的快速隆升事件,三期隆升导致的地层剥蚀量分别为227m、593m和865m;东海陆架盆地经历了古新世末-始新世初（~56Ma）、始新世末-渐新世初（~32Ma）和晚中新世（~10Ma）三期构造反转,三期反转导致的局部地层最大剥蚀量分别可达1200m、1300m和2000m。在时间上,东海陆架盆地的始新世末-渐新世初（~32Ma）和晚中新世（~10Ma）的构造反转分别滞后于浙江的晚始新世（34.5~33.5Ma）和中中新世（16~11.5Ma）的隆升时间,说明这两期挤压-剥蚀事件分别具有自西向东的迁移性,即印度-欧亚板块碰撞的远程效应可能是导致该迁移特征的原因;在强度上,东海陆架盆地的反转剥蚀量大于浙江境内的地层隆升量、挤压强度东强西弱,中新世晚期菲律宾海板块向西俯冲导致冲绳海槽弧后伸展产生向西的挤压力、这种挤压应力向陆内传递且强度变弱可能是导致该特征的原因。

     

青藏高原地热资源与地壳热结构

青藏高原具有独特的地壳结构和高热背景。南部的喜马拉雅地块属于"热壳冷幔"型,拉萨-冈底斯地体属于"热壳热幔"型地块,该区域内中地壳范围内存在一低速高导层,可能为部分熔融岩浆囊,形成了规模宏伟的地热带。高原水热活动带主要出露在喜马拉雅-冈底斯-念青唐古拉之间,>25℃的水热区有283处,>80℃的沸、热泉有近40处。著名的羊八井高温热储地热田,已经建成装机容量达25.18 MW的地热电站,为拉萨输送了大量电力,地热资源在高原能源结构中占有重要的地位,具有巨大的开发前景和价值。      

东南大陆边缘早侏罗世火成岩特征及其构造意义

东南大陆边缘早侏罗世火成岩主要呈双峰式火山岩、基性超基性杂岩体及A型花岗岩等形态产出。本文运用岩石学探针技术,通过早侏罗世火成岩岩石学与地球化学研究,并与晚中生代火成岩作对比,提出早侏罗世火成岩的形成与南岭东段近EW向张性断裂活动有关,标志着印支挤压造山的结束;之后东南大陆进入晚中生代NE向活动大陆边缘俯冲造山阶段,经历了挤压造山—剪切拉张过程,并在晚白垩世末期进入又一轮后造山拉张裂解阶段,即中生代时东南大陆边缘经历了早中生代(三叠纪—早侏罗世)和晚中生代(中侏罗世—晚白垩世)两期造山事件,其中早侏罗世的区域拉张作用是特提斯构造域向滨太平洋构造域转换的前奏,构造域转换可能始于中侏罗世(165Ma)。     

Heat Aggregation Mechanisms of Hot Dry Rocks Resources in the Gonghe Basin,Northeastern Tibetan Plateau

Hot dry rock (HDR) is an important geothermal resource and clean energy source that may play an increasingly important role in future energy management. High-temperature HDR resources were recently detected in deep regions of the Gonghe Basin on the northeastern edge of the Tibetan Plateau, which led to a significant breakthrough in HDR resource exploration in China. This research analyzes the deep temperature distribution, radiogenic heat production, heat flow, and crustal thermal structure in the Qiaboqia Valley, Guide Plain, and Zhacanggou area of the Gonghe Basin based on geothermal exploration borehole logging data, rock thermophysical properties, and regional geophysical exploration data. The results are applied to discuss the heat accumulation mechanism of the HDR resources in the Gonghe Basin. The findings suggest that a low-velocity layer in the thickened crust of the Tibetan Plateau provides the most important source of constant intracrustal heat for the formation of HDR resources in the Gonghe Basin, whereas crustal thickening redistributes the concentrated layer of radioactive elements, which compensates for the relatively low heat production of the basal granite and serves as an important supplement to the heat of the HDR resources. The negative effect is that the downward curvature of the lithospheric upper mantle caused by crustal thickening leads to a small mantle heat flow component. As a result, the heat flows in the Qiaboqia Valley and Guide Plain of the Gonghe Basin are 106.2 and 77.6 mW/m2, respectively, in which the crust-mantle heat flow ratio of the former is 3.12:1, indicating a notably anomalous intracrustal thermal structure. In contrast, the crust-mantle heat flow ratio in the Guide Plain is 1.84:1, which reflects a typical hot crust-cold mantle thermal structure. The Guide Plain and Zhacanggou area show the same increasing temperature trend with depth, which reflects that their geothermal backgrounds and deep high-temperature environments are similar. These results provide important insight on the heat source mechanism of HDR resource formation in the Tibetan Plateau and useful guidance for future HDR resource exploration projects and target sites selection in similar areas.     

从青海共和—贵德盆地与山地地温场特征探讨热源机制和地热系统

青海共和—贵德盆地及其相间山地具有盆地传导型地热资源,地温梯度大,地热勘探钻孔在基底均见花岗岩,盆缘山地隆起断裂对流型温泉呈带分布,水温高,也出露在花岗岩中.对其热源机制的认识目前存在分歧.本文对地幔型热源提出质疑,认为花岗岩放射性生热为壳内热源并提出地化依据;同时,用地热钻孔测温曲线和地球化学地热温标对热储温度和深度进行了探讨.研究结果表明,周边山地属中温地热系统,新生代断陷盆地内具高温地热系统,其钻孔井底测温已达175~180℃,是干热岩开发的优选地段.     

Shallow geothermal regime in the Perth Metropolitan Area

Exploration of Perth's geothermal potential has been performed by the Western Australian Geothermal Centre of Excellence (WAGCoE). Detailed vertical temperature and gamma ray logging of 17 Western Australia Department of Water's (DoW) Artesian Monitoring (AM) wells was completed throughout the Perth Metropolitan Area (PMA). In addition, temperature logs from 53 DoW AM wells measured in the 1980s were digitised into LAS format. The logged data are available in the WAGCoE Data Catalogue.

Analysis of the gamma ray logs yielded the first estimates of radiogenic heat production in Perth Basin formations. Values by formation ranged between 0.24 and 1.065 μW m^?3. The temperature logs provide a picture of true formation temperatures within shallow sediments in the Perth Basin. A three-dimensional model of the temperature distribution was used to produce maps of temperature at depth and on the top of the Yarragadee aquifer.

The temperature data were interpreted with a one-dimensional conductive heat model. Significant differences between the model and the observations was indicative of heat moving via non-conductive mechanisms, such as advection or convection. Evidence of non-conductive or advective heat flow is demonstrated in most formations in the region, with significant effects in the aquifers. Average conductive geothermal gradients range from 13°C km^?1 to 39°C km^?1, with sandstone formations exhibiting average gradients of approximately 25°C km^?1, while insulating silt/shale formations show higher average gradients of over 30°C km^?1.

To produce preliminary heat flow estimates, temperature gradients were combined with thermal conductivities measured elsewhere. The geometric mean heat flow estimates range between 64 mW m^?2 to 91 mW m^?2, with the standard deviation of the arithmetic mean heat flow ranging between 15 and 23 mW m^?2.

The study characterises the shallow temperature regime in the Perth Metropolitan Area, which is of direct relevance towards developing commercial geothermal projects.     

Heat flow and crustal thermal structure in the Late Archaean Closepet Granite batholith,south India

The Late Archaean Closepet Granite batholith in south India is exposed at different crustal levels grading from greenschist facies in the north through amphibolite and granulite facies in the south along a ∼400 km long segment in the Dharwar craton. Two areas, Pavagada and Magadi, located in the Main Mass of the batholith, best represent the granitoid of the greenschist and amphibolite facies crustal levels respectively. Heat flow estimates of 38 mW m⁻² from Pavagada and 25 mW m⁻² from Magadi have been obtained through measurements in deep (430 and 445 m) and carefully sited boreholes. Measurements made in four boreholes of opportunity in Pavagada area yield a mean heat flow of 39 ± 4 (s.d.) mW m⁻², which is in good agreement with the estimate from deep borehole. The study, therefore, demonstrates a clear-cut heat flow variation concomitant with the crustal levels exposed in the two areas. The mean heat production estimates for the greenschist facies and amphibolite facies layers constituting the Main Mass of the batholith are 2.9 and 1.8 μW m⁻³, respectively. The enhanced heat flow in the Pavagada area is consistent with the occurrence of a radioelement-enriched 2-km-thick greenschist facies layer granitoid overlying the granitoid of the amphibolite facies layer which is twice as thick as represented in the Magadi area. The crustal heat production models indicate similar mantle heat flow estimates in the range 12–14 mW m⁻², consistent with the other parts of the greenstone-granite-gneiss terrain of the Dharwar craton.     

大地热流研究揭示的中国地壳成分横向变化

依据大地热流值、地壳厚度以及大陆壳／幔热流比与地下流体氦同位素比值的相关关系，计算出中国主要构造单元地壳生热率。同时，根据Rudnick和Fountain(1995）的数据得到地壳生热率和SiO2质量分数的线性关系，进而利用生热率数据得到地壳SiO2质量分数。此方法得到的中国东部地壳生热率和SiO2质量分数与基于地震波速的成分模型相符。中国大陆地壳生热率和SiO2质量分数横向变化明显，东部地区地壳为中性成分，相对富集强不相容元素；而西北部盆地地壳成分偏于中基性。华北、扬子和塔里木地壳成分差异较大，克拉通内部表现出明显的成分非均匀性，褶皱带地壳一般较克拉通略富长英质组分。     

江西芦溪县南部大地热流特征

江西省芦溪县南部地区地热资源丰富, 但地热地质研究程度较低, 大地热流测量工作进行的较少, 制约着区域地热资源勘查开发。本文以芦溪县南部的新泉和石溪为研究区, 结合钻孔岩心热物性测试和地温测井等分析了研究区岩石热导率、地温场、热源机制的特征。研究区岩石热导率平均值为 2.063~6.176 W/(m·K), 热导率最高的为硅质石英岩, 可作为良好的导热岩体。大地热流平均值为 76.39 mW/m2, 远高于中国大陆地区的平均值62.5 mW/m2, 该地区具有较高的热背景值。花岗岩放射性生热率平均值为2.16 μW/m3, 不属于高产热型岩体, 放射性生热对地表热流贡献较小, 热源来源为地壳深部供热。研究区构造活动强烈, 深大断裂和次级断裂发育, 为地下热水的深部循环提供了良好的导热和导水通道。本研究可为武功山地区的地热资源开发提供重要启示。     

广东惠州黄沙洞地区岩石圈热-流变结构及其热源启示

岩石圈热-流变结构研究是揭示岩石圈范围内热状态的有效手段,开展地热异常区的岩石圈热-流变结构研究可以对热源贡献进行有效约束。东南沿海地区是我国地热资源重要分布区,地表出露大量天然温泉,地热钻探揭露深部具有较高的地温梯度,然而关于其热源机制尚未有定论,且深部是否赋存干热岩资源亦不清楚。以广东惠州黄沙洞地热田为研究对象,分析岩石圈尺度温度分布和流变强度,探讨黄沙洞地热田的热源构成,分析浅部水热系统的热影响,并对干热岩资源前景进行分析。结果表明：（1）黄沙洞地热田水热活动影响下地表热通量为130.3 mW/m2,地壳热流与地幔热流值相近,表现为温壳温幔型岩石圈热结构,此外,构造活动相关热流达到了30.5~60.3 mW/m2;（2）岩石圈流变结构显示中地壳存在韧性流变层,上地壳与下地壳以脆性破裂为主,下地壳与地幔表现出流变结构耦合,为相对稳固的地壳底界;（3）黄沙洞地热田的热源以地壳构造活动产生的热源为主,地幔热源和放射性生热是主要的热源组成部分,构造热作用的主要方式包括区域深断裂的热聚敛和水热系统循环换热,两者可能通过“接力式”热传递携带热量至浅表;（4）区域深断裂的热聚敛在构造热作用中的占比是影响干热岩资源前景的关键因素。本项研究可为后续东南沿海同类型地区的干热岩资源勘查与靶区选址提供参考。     

Seismically constrained two-dimensional crustal thermal structure of the cambay basin

The temperature field within the crust is closely related to tectonic history as well as many other geological processes inside the earth. Therefore, knowledge of the crustal thermal structure of a region is of great importance for its tectonophysical studies. This work deals with the two-dimensional thermal modelling to delineate the crustal thermal structure along a 230 km long Deep Seismic Sounding (DSS) profile in the north Cambay basin. In this work P-wave velocities obtained from the DSS studies have been converted into heat generation values for the computation of temperature distribution. The model result reveals the Curie isotherm at a depth of ≈22 km and Moho temperature at around 900‡C.     

The thermal structure and thickness of continental roots

We compare heat flow data from the Precambrian shields in North America and in South Africa. We also review data available in other less well-sampled Shield regions. Variations in crustal heat production account for most of the variability of the heat flow. Because of this variability, it is difficult to define a single average crustal model representative of a whole tectonic province. The average heat flow values of different Archean provinces in Canada, South Africa, Australia and India differ by significant amounts. This is also true for Proterozoic provinces. For example, the heat flow is significantly higher in the Proterozoic Namaqua–Natal Belt of South Africa than in the Grenville Province of the Canadian Shield (61 vs. 41 mW m⁻² on average). These observations indicate that it is not possible to define single value of the average heat flow for all provinces of the same crustal age. Large amplitude short wavelength variations of the heat flow suggest that most of the difference between Proterozoic and Archean heat flow is of crustal origin. In eastern Canada, there is no good correlation between the local values of heat flow and heat production. In the Archean, Proterozoic and Paleozoic provinces of eastern Canada, heat flow values through rocks with the same heat production are not significantly different. There is therefore no evidence for variations of the mantle heat flow beneath these different provinces. After removing the local crustal heat production from the surface heat flow, the mantle (Moho) heat flow was estimated to be between 10–15 mW m⁻² in the Archean, Proterozoic and Paleozoic provinces of eastern Canada. Estimates of the mantle heat flow in the Kaapvaal craton of South Africa may be slightly higher (≈17 mW m⁻²). Large-scale variations of bulk crustal heat production are well-documented in Canada and imply significant differences of deep lithospheric thermal structure. In thick lithosphere, surficial heat flow measurements record a time average of heat production in the lithospheric mantle and are not in equilibrium with the instantaneous heat production. The low mantle heat flow and current estimates of heat production in the lithospheric mantle do not support a mechanical (conductive) lithosphere thinner than 200 km and thicker than 330 km. Temperature anomalies with surrounding oceanic mantle extend to the convective boundary layer below the conductive layer, and hence to depths greater than these estimates. Mechanical and thermal stability of the lithosphere require the mantle part of the lithosphere to be chemically buoyant and depleted in radiogenic elements. Both characteristics are achieved simultaneously by partial melting and melt extraction.