新密煤田地热资源成因探讨     

张春陆  蔡敦峰 《中国煤田地质》2005,17(6):29-31

通过对新密煤田地质条件、构造条件、煤系岩石的放射性特征、下热水的水文地球化学、气体成分等特征的研究,认为形成新密煤田地热资源的热源是来自硫化矿物生热、岩浆余热以及煤系地层岩石放射性物质产热的学说证据不足;而新密煤田的水文地质条件,地质构造条件为该区地下水的深循环提供了条件,故而在该区形成了水热型的中低温地热资源.  相似文献   

中国大陆科学钻探（CCSD）主孔地区岩石圈热结构   总被引：11，自引：2，他引：11  

吴耀  金振民  欧新功  徐海军  王璐 《岩石学报》2005,21(2):439-450

岩石圈热结构是指地球内部热量在壳幔的配分比例、温度以及热导率和生热率等热学参数在岩石圈中的分布特征。岩石圈的热结构直接影响着岩石的物理性质和流变学性质,同时还控制了化学反应的类型和速度,从而制约着岩石圈的发展和演化。本文在前人CCSD主孔岩石主、微量元素研究基础上,利用Rybach生热率公式计算了钻孔岩石的放射性生热率,并结合岩石热导率的测定研究了CCSD主孔100-2000m岩石的热结构和主孔榴辉岩在不同退变质程度下生热率、热导率的变化:钻孔中岩石的平均生热率为0.95μWm-3,平均热导率为2.96mWm-1K-1。,其中片麻岩生热率高迭1.01-1.7μWm-3,热导率为2.76-2.96mWm-1K-1;基性超基性岩石生热率最低(<0.21μWm-3),热导率则高达3.20mWm-1K-1以上;新鲜榴辉岩生热率、热导率居中,分剐为0.16-0.44μWm-3和3.31-3.85mWm-1K-1。钻孔中榴辉岩生热率、热导率变化主要受岩性控制:从新鲜榴辉岩到完全退变榴辉岩,热导率总体上降低,但从强退变榴辉岩到完全退变榴辉岩,岩石热导率升高;而在此过程中岩石生热率总体上升高,仅当从中等退变质榴辉岩退变为强退变质榴辉岩时,岩石生热率出现降低趋势。在综合研究的基础上预测CCSD主孔5000m深度处温度为139℃,温度范围为131-151℃。根据区域深部地球物理探测成果对CCSD主孔地区岩石圈热结构进行了研究:上地壳底部温度为256℃,中地壳底部温度为492℃,Moho面温度为683℃,岩石圈底部温度为1185℃,来自地幔的热流为44.1mWm-2,对地表热流的贡献率为58%。研究结果表明,由岩石物理方法获得的CCSD主孔地区岩石圈地温曲线与石榴石-二辉橄榄岩包体推断的中国东部地温曲线十分吻合,本文从实验岩石物理学角度为CCSD主孔地区岩石圈热结构研究提供了重要约束  相似文献   

青藏高原对其东北侧干旱形成的数值试验   总被引：4，自引：5，他引：4  

王咏青  陈联寿  罗哲贤 《高原气象》2002,21(6):529-535

应用再分析资料，指出高原边界层内存在北高南低偶极子型涡旋对的独特气候现象。根据当雄站1998年5月31日至6月4日感热通量的连续观测资料，确定了高原热力作用的时变特征，分别用不同的理想高原初始涡度场加定常热源强迫和时变热源强迫代入正压准地转涡度模式，研究了高原东北侧干旱的形成。认为有三种过程在起着重要作用，它们是：基流对上游反气旋涡旋的平流输送、南侧气旋涡旋的能量频散以及高原热力强迫引起的频散生成高值系统的增强。  相似文献   

滇西上芒岗红色粘土型金矿的元素地球化学特征及其物质来源探讨     

饶文波  高振敏  杨竹森  罗泰义  李红阳  陶琰  谱传杰 《地球化学》2002,31(6):577-586

对滇西上芒岗红色粘土型金矿的主元素，微量元素和稀土元素地球化学特征进行了详细的研究。结果表明，主元素Al2O3,Fe2O3和K2O在红色粘土剖面中共迁移同沉淀，SiO2的变化却与它们相反，这揭示了上芒岗红色粘土型金矿的红色粘土层除了残积带红土化程度高外，总体上SiO2含量高，去硅作用不完全，红土化程度低；与地层，矿化蚀变岩的对比分析结果表明，红色粘土是在加勐嘎组泥岩基础上经红土化作用形成的，红色粘土的微量元素表现为Au,Hg,As,Sb,Cu,Pb,Zn和Mo等元素的共生,在红土化好的残积带明显富集；红色粘土的大离子元素分布模式与矿化蚀变岩和嘎组的相似，红色粘土的稀土分布模式与矿化蚀变岩和地层的相似，表现为轻稀土富集的右倾型平缓曲线，稀土元素分蚀明显的地方金富集，以上分析揭示，此金矿的成矿物质主要来自矿化蚀变岩，红色粘土主要来源于勐嘎组和矿化蚀变岩。  相似文献   

湘中锡矿山锑矿床成矿物质来源的同位素示踪   总被引：14，自引：0，他引：14  

彭建堂  胡瑞忠  邹利群  刘建雄 《矿物学报》2002,22(2):155-159

本文利用放射成因同位素（Pb、Sr)和轻稳定同位素（C、O）对锡矿山超大型锑矿床的成矿物质来源进行了示踪，从物源角度揭示了其在规模成矿、元素发生超常富集的原因。研究表明，锡矿山锑矿床的成矿物质不可能是来自赋矿围岩；深部地幔和基底都卷入了该矿的成矿作用；富Sb的交代型地幔和富Sb的元古界基底为其大规模成矿提供了充足的矿源，两者是形成锡成山超大型锑矿床的前提条件。  相似文献   

富碱斑岩中超镁铁深源包体岩石的矿物学特征   总被引：10，自引：0，他引：10  

刘显凡  刘家铎  阳正熙  张成江  吴德超  李佑国 《矿物学报》2002,22(3):289-295

在云南省鹤庆县六合乡富碱斑岩体中找到超镁铁深源岩石包体，这对于研究富碱斑岩的起源和演化及其成岩成矿作用具有重要意义。本文较系统地研究了深源包体岩石的矿物学特征，揭示该深源包体具有原始上地幔岩在地幔条件下受到一定程度富集地幔流体交代作用改造的特征，具有富集地幔低程度部分熔融属性，为富碱斑岩的成岩成矿演化提供了重要的矿物学依据。  相似文献   

The Mw = 6.0, 7 September 1999 Athens Earthquake     

Papadimitriou  P.  Voulgaris  N.  Kassaras  I.  Kaviris  G.  Delibasis  N.  Makropoulos  K. 《Natural Hazards》2002,27(1-2):15-33

On 7 September 1999 at 11:56 GMT a destructive earthquake (M_w = 6.0) occurred close to Athens (Greece). The rupture process is examined using data from the Cornet local permanent network, as well as teleseismic recordings. Data recorded by a temporary seismological network were analyzed to study the aftershock sequence. The mainshock was relocated at 38.105°N, 23.565°E, about 20 km northwest of Athens. Four foreshocks were also relocated close to the mainshock. The modeling of teleseismic P and SH waves provides a well-constrained focal mechanism of the mainshock (strike = 105°, dip = 55° and rake = -80°) at a depth of 8 km and a seismic moment M₀ = 1.010²⁵ dyn·cm. The obtained fault plane solution represents normal faulting indicating an almost north-south extension. More than 3500 aftershocks were located, 1813 of which present RMS < 0.1 s and ERH, ERZ < 1.0 km. Two main clusters were distinguished, while the depth distribution is concentrated between 2 and 11 km. Over 1000 fault plane solutions of aftershocks were constrained, the majority of which also correspond to N–S extension. No surface breaks were observed but the fault plane solution of the mainshock is in agreement with the tectonics of the area and with the focal mechanisms obtained by aftershocks. The hypocenter of the mainshock is located on the deep western edge of the fault plane. The relocated epicenter coincides with the fringe that represents the highest deformation observed on the differential interferometric image. The calculated source duration is 5 sec, while the estimated dimensions of the fault are 15 km length and 10 km width. The source process is characterized by unilateral eastward rupture propagation, towards the city of Athens. An evident stop phase observed in the recordings of the Cornet local stations is interpreted as a barrier caused by the Aegaleo Mountain.  相似文献   

Heat flow and thermal modeling of the Yinggehai Basin, South China Sea   总被引：9，自引：0，他引：9  

Lijuan He  Liangping Xiong  Jiyang Wang 《Tectonophysics》2002,351(3)

Geothermal gradients are estimated to vary from 31 to 43 °C/km in the Yinggehai Basin based on 99 temperature data sets compiled from oil well data. Thirty-seven thermal conductivity measurements on core samples were made and the effects of porosity and water saturation were corrected. Thermal conductivities of mudstone and sandstone range from 1.2 to 2.7 W/m K, with a mean of 2.0±0.5 W/m K after approximate correction. Heat flow at six sites in the Yinggehai Basin range from 69 to 86 mW/m², with a mean value of 79±7 mW/m². Thick sediments and high sedimentation rates resulted in a considerable radiogenic contribution, but also depressed the heat flow. Measurements indicate the radiogenic heat production in the sediment is 1.28 μW/m³, which contributes 20% to the surface heat flow. After subtracting radiogenic heat contribution of the sediment, and sedimentation correction, the average basal heat flow from basement is about 86 mW/m².Three stages of extension are recognized in the subsidence history, and a kinematic model is used to study the thermal evolution of the basin since the Cenozoic era. Model results show that the peak value of basal heat flow was getting higher and higher through the Cenozoic. The maximum basal heat flow increased from 65 mW/m² in the first stage to 75 mW/m² in the second stage, and then 90 mW/m² in the third stage. The present temperature field of the lithosphere of the Yinggehai Basin, which is still transient, is the result of the multistage extension, but was primarily associated with the Pliocene extension.  相似文献   

Stability of earthquake moment tensor inversions: effect of the double-couple constraint   总被引：1，自引：0，他引：1  

C. Henry  J. H. Woodhouse  S. Das   《Tectonophysics》2002,356(1-3)

We show that spurious large non-double-couple components can be obtained in inversions for the full deviatoric moment tensor for shallow crustal earthquakes due to inaccurate Earth models. The traditional “best double-couple” solution does not in general provide an optimal estimate of a double-couple mechanism, and is only reliable when the non-double-couple component of the full deviatoric solution is small. The inverse problem for the moment tensors of the 1998 Antarctic Plate and 2000 Wharton Basin strike-slip earthquakes is shown in each case to have two well-fitting minima in the misfit function of pure double-couple solutions. Such pairs of solutions are most likely to exist for earthquakes which are close either to vertical strike-slip or to dip-slip on a fault plane dipping at 45°. It is shown theoretically that these pairs of solutions arise from the combination of the pure double-couple constraint and the instability of two elements of the moment tensor. No significant non-double-couple component is found for the shallow thrusting 1996 Biak, Indonesia earthquake.  相似文献   

Low-temperature thermodynamic properties of disordered zeolites of the natrolite group     

I. E. Paukov  N. K. Moroz  Yu. A. Kovalevskaya  I. A. Belitsky 《Physics and Chemistry of Minerals》2002,29(4):300-306

 The heat capacity of paranatrolite and tetranatrolite with a disordered distribution of Al and Si atoms has been measured in the temperature range of 6–309 K using the adiabatic calorimetry technique. The composition of the samples is represented with the formula (Na_1.90K_0.22Ca_0.06)[Al_2.24Si_2.76O₁₀]·nH₂O, where n=3.10 for paranatrolite and n=2.31 for tetranatrolite. For both zeolites, thermodynamic functions (vibrational entropy, enthalpy, and free energy function) have been calculated. At T=298.15 K, the values of the heat capacity and entropy are 425.1 ± 0.8 and 419.1 ±0.8 J K⁻¹ mol⁻¹ for paranatrolite and 381.0 ± 0.7 and 383.2 ± 0.7 J K⁻¹ mol⁻¹ for tetranatrolite. Thermodynamic functions for tetranatrolite and paranatrolite with compositions corrected for the amount of extraframework cations and water molecules have also been calculated. The calculation for tetranatrolite with two water molecules and two extraframework cations per formula yields: C _p (298.15)=359.1 J K⁻¹ mol⁻¹, S(298.15) −S(0)=362.8 J K⁻¹ mol⁻¹. Comparing these values with the literature data for the (Al,Si)-ordered natrolite, we can conclude that the order in tetrahedral atoms does not affect the heat capacity. The analysis of derivatives dC/dT for natrolite, paranatrolite, and tetranatrolite has indicated that the water- cations subsystem within the highly hydrated zeolite may become unstable at temperatures above 200 K. Received: 30 July 2001 / Accepted: 15 November 2001  相似文献