共查询到10条相似文献，搜索用时 296 毫秒
1.
中国东北地区地热资源及热结构分析 总被引：1，自引：0，他引：1
在我国东北地区，盆地的热流高而在山区和地台区（额尔古纳和佳木斯地台）热流较低，通过对该区的研究发现，在地壳和上地幔中莫霍面埋深，高导层埋深和热流值之间存在着密切的联系，通过对该区热流数据分析我们可以得到这样的结论：该区的地壳和上地幔的热结构引起了热流分布的变化。计算结果还表明，该区地台的地幔热流，地壳中10km以下和10km以上的热流对地表热流的贡献不同。该区松辽盆地中广泛分布着传导型中低温地热资源，对松辽盆地地热资源的开发利用有着广泛的前景。最后结合已有的地质和物探资料，还给出了长白山天池火山地区长白温泉地热系统的概念性模型。 相似文献
2.
济阳坳陷地幔热流和深部温度 总被引：8，自引：2，他引：6
济阳坳陷深部地热状况对于分析岩石圈深部结构特征、探索该盆地形成和演化的地球动力学过程具有重要意义.依据济阳坳陷最新的钻探资料和深部地球物理探测结果, 按沉积盖层、上、中、下地壳4层结构, 建立了分别代表该区凹陷部位和凸起及斜坡带上的2种地壳结构模型.通过多道能谱分析, 测试了区内4 3块岩心样品的放射性元素U、Th、40K含量, 统计得出了济阳坳陷沉积盖层的平均生热率为(1.40±0.26) μW/m3.在研究大地热流分布的基础上, 结合济阳坳陷地壳各岩层放射性生热率, 采用“剥层”法, 从地表开始, 由浅到深逐步扣除各层段所提供的热量, 得到了济阳坳陷的地幔热流.并且采用相似的方法, 利用一维稳态热传导方程, 分析了地壳上地幔顶部的温度状况.结果表明, 济阳坳陷的地幔热流约为38.4~39.2 mW/m2, 占整个地表总热流量的5 8%;地幔顶部温度约为602~636℃.与世界上其他各类地质构造单元相比, 济阳坳陷无论是地幔热流值或其与地表热流之比值都是比较高的, 其深部地热状态具有介于稳定地区和构造活动区之间的特点. 相似文献
3.
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
4.
从1974年至今,人们对青藏高原的研究积累了大量的地球物理资料。笔者搜集了23条地震剖面纵波数据,利用地震纵波速度和生热率的关系,绘制了各条剖面的地壳岩石生热率随深度变化的等值线,并结合已有的大地热流数据,得到了地幔热流密度分布情况。从地幔热流密度分布可以看出:在班公—怒江缝合带、印度—雅鲁藏布江缝合带、拉萨地体上存在地幔热流较高区域;该区域位于地块碰撞挤压带上,地层构造复杂,地热资源丰富,以著名的羊八井地热田为代表。初步推断该区域地幔岩浆较活跃。 相似文献
5.
The thermal structure and thickness of continental roots 总被引：19，自引：0，他引：19
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. 相似文献
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.
蒙古—贝加尔裂谷的演化及其形成的动力学机制一直是地学界争论的焦点。至今,对其地热学的相关研究一直比较匮乏。本文根据前人对蒙古—贝加尔及邻区的独特地貌、构造和玄武岩火山岩浆作用的研究,并结合现今地表大地热流特征共同探讨了其地球动力学机制。根据最新大地热流分布特征表明:蒙古地区的高热流区(120 mW/m~2)主要集中在蒙古Hangay穹窿北部Hovsgol裂谷及其周围裂谷内;贝加尔裂谷整体热流都较高,且贝加尔东北部热流达160 mW/m~2以上(比前人报道的更高),其中部热流也高(120 mW/m~2)。综合地热、地质与地球物理成果,本文认为晚新生代的地幔柱对蒙古—贝加尔地区的形成起着重要作用。 相似文献
8.
LIN Wenjing WANG Guiling ZHANG Shengsheng ZHAO Zhen XING Linxiao GAN Haonan TAN Xianfeng 《《地质学报》英文版》2021,95(6):1793-1804
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. 相似文献
9.
浙闽粤东部地热场研究及其意义 总被引：5，自引：0，他引：5
根据研究区的现今地表温泉温度、地温梯度、地表热流值及地壳结构，恢复了古地热场，计算了各期岩浆活动产生的瞬时古地温梯度，初步探讨了研究区的热源及有机质热演化史。指出地幔热流是控制区域性地热场的主要因素，岩浆热流控制了局部高地热场的分布，构造活动产生的剪切热流对俯冲带及剪切带的瞬时古地热场有重要影响。研究区的有机质成熟度在总体处于过成熟的背景下，仍存在局部的成熟或成熟晚阶段的异常区，有可能成为最重要的 相似文献
10.
In this paper the effect of transient uplift/erosion on the relationship between surface heat flow and heat generation for
truncated exponential model of radiogenic heat source distribution and basal asthenospheric convection is investigated. Asthenospheric
convection is described by a parameterized model, in the form of a nonlinear heat flux boundary condition involving basal
temperature and mantle internal temperature. This boundary condition has been linearized and the analytical solution of the
problem is obtained by the eigenvalue-eigenfunction expansion method. The analytical solution is used to derive the nature
of surface heat flow and heat generation relationship. The results show that the linear relationship is maintained during
the uplift/erosion and the estimates of the slope of the linear relationship are different from the depth scale of the exponential
model and increase with the rate of uplift/erosion. The estimates of the reduced heat flow also increase with the rate of
uplift/erosion. These results would find applications in the interpretation of linear surface heat flow and heat generation
relationship which is observed in different tectonic environment. 相似文献