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1.
板片俯冲过程将地表碳带入地球内部,火山作用将深部碳输送至地球外部圈层,两者构成了地球深部碳循环的主要方式,进而影响了地史时期的气候变化。我国东北新生代火山活动被认为是太平洋板片深俯冲作用的产物,板片俯冲导致岩浆源区强烈的碳酸盐组分交代作用,进而使东北亚上地幔成为一个新生代时期的巨型深部碳库,它的活动和释放将会对全球的气候与环境变化造成重要影响。然而,有关该深部碳库向当今大气圈输送CO_2气体的规模及其演化过程尚不清楚,从而影响了进一步定量评估该碳库在全球变化研究中的地位和作用。针对上述科学问题,本文对我国东北长白山、五大连池和阿尔山火山释放CO_2气体的规模与成因进行了研究。结果表明,东北新生代火山区的土壤CO_2释放通量介于9.6～41.2g·m~(-2)·d~(-1)之间,每年向当今大气圈释放CO_2气体约为2.1Mt(其中,长白山火山区为0.94Mt,五大连池火山区为1.2Mt)。气体地球化学研究证实,长白山与五大连池火山气体均起源于太平洋板片深俯冲环境;但是,与长白山相比,五大连池火山气体具有较高比例壳源组分贡献。阿尔山火山气体的成分与长白山和五大连池火山区存在着明显的差异,它们以N_2为主( 95%),并且其δ~(15)N_(N_2)值高于空气值(1.3‰～1.9‰),~3He/~4He比值较低(0.14～0.18R_A),δ~(13)C_(CO_2)较轻(-13.7‰～-6.2‰),表明壳源富氮有机沉积物的贡献占比较大的比例。上述特征进一步表明,阿尔山火山气体在上升经过地下水时可能滞留了较长时间,混染了大量的陆壳组分,其源区并未受到太平洋板片俯冲物质的显著影响。 相似文献
2.
高温地热区土壤微渗漏的温室气体释放通量研究: 以藏南羊八井地热田为例 总被引：1，自引：1，他引：0
土壤微渗漏是地球深部的构造-岩浆活动向大气圈释放温室气体的重要形式之一。近年来,国外许多地热区已经开展了土壤微渗漏温室气体释放通量的定量研究,然而,目前我国尚无该方面的系统研究报道。本文阐述了利用密闭气室法测量地热区土壤微渗漏温室气体释放通量的方法和原理,并将其应用于青藏高原的羊八井地热田。根据研究区的地热活动强度,将羊八井地热田划分为土壤微渗漏释放较弱的A区和土壤微渗漏释放较强的B区。计算结果表明,A区和B区的CO2气体释放通量分别为6.7g·m-2·day-1和98.5g·m-2·day-1。两区释放通量的差异主要受控于断裂的发育程度,即A区位于裂谷的中部,断裂发育程度较差,B区靠近念青唐古拉正断层,断裂发育程度较高,为温室气体的逸出提供了良好的运移通道。羊八井地热田土壤微渗漏CO2气体的释放总量约为8.6×104t·a-1,接近于意大利Vulcano火山区的土壤微渗漏温室气体释放规模(1×105t·a-1)。研究区的气体同位素组分测试结果显示,He同位素值介于0.107RA~0.648RA(RA为大气3He/4He比值),δ13C值介于-11.33‰~-6.79‰(vs.PDB),表明羊八井地热田的温室气体可能主要来源于大陆俯冲环境下的加厚陆壳,其温室气体释放通量的规模主要受控于地壳的岩浆活动以及南北向裂谷拉张作用。羊八井地热田所在的拉萨地块是青藏高原温室气体释放活动最强烈的区域之一,以往的研究表明,青藏高原出露大量新生代火山、地热区,开展火山、地热区温室气体释放通量的研究将有助于深入理解地质因素向当今大气圈释放温室气体的规模等与深部碳循环相关的科学问题。 相似文献
3.
不同构造域的火山释放CO_2气体的方式、机制和规模具有明显的差异。在全球变暖的大背景下,定量化研究不同类型火山区CO_2气体的释放通量、模拟及计算火山气体的来源演化,对于估算地质源温室气体释放对大气圈温室气体增加的贡献,以及理解地球的深部碳循环过程具有重要意义。近年来,全球火山区CO_2气体释放研究取得了显著进展,尤其在定量研究火山区CO_2气体释放通量的方法、气体源区与地球动力学背景的判定以及不同构造背景的火山区CO_2气体释放特征等领域取得了重大成果。本文综述了不同构造域火山区CO_2气体释放研究的最新成果,详细介绍了我国新生代典型火山地热区的CO_2气体释放研究进展。 相似文献
4.
腾冲新生代火山区温泉CO2气体排放通量研究 总被引：6，自引：6，他引：0
近期研究表明,不仅火山喷发期会向当时的大气圈输送大量的温室气体,火山间歇期同样会释放大量的温室气体。在火山活动间歇期,火山区主要以喷气孔、温(热)泉以及土壤微渗漏等形式向大气圈释放温室气体。腾冲是我国重要的新生代火山区,同时也是重要的水热活动区,那里出露大量的温泉,然而目前未见腾冲火山区温泉气体排放通量的研究报道。本文利用数字皂膜通量仪测量了腾冲新生代火山区温泉中CO2的排放通量。研究结果表明,腾冲新生代火山区温泉向当今大气圈输送的CO2通量达3.58×103 t·a-1,相当于意大利锡耶纳Bassoleto地热区温泉中CO2的排放规模。腾冲火山区温泉的CO2释放通量主要受深部岩浆囊、断裂分布、地下水循环、围岩成分等多方面因素的影响。本文根据温泉中CO2的排放特征,将腾冲温泉分为南北两区,南区温泉CO2通量远高于北区的温泉,热海地热区的通量为腾冲CO2通量的最大值。在北温泉区,CO2通量主要受控于断裂的分布;而在南温泉区,除受到断裂控制外,热海地热区底部的岩浆囊及其与围岩的相互作用成为CO2气体的重要物质来源,同时高温的岩浆囊为温泉及CO2的形成提供了重要热源。 相似文献
5.
温度是岩浆囊的重要物理参数,获取温度参数并监测其变化对更好地理解岩浆囊的物理化学性质和行为、评价火山的活动性和喷发危险性具有重要的理论和现实意义。火山岩浆-水热系统丰富的含碳气体,这些含碳气体间碳同位素温度计为我们解决休眠火山区地下岩浆囊的温度问题提供了可能。我们对宁洱火山区地表地热异常强度最高区的4个温泉点CO_2、CH_4碳同位素组成进行了2年的连续观测和2次平行观测,利用观测数据对CO_2、CH_4气体的岩浆来源进行了甄别,对CO_2-CH_4间碳同位素分馏是否发到平衡进行了判断,然后利用Horita CO_2-CH_4碳同位素平衡分馏方程计算了宁洱-通关火山区逸出气体的源区温度。结果表明:宁洱火山区4个样点中,1个样点的CO_2和CH_4均为非岩浆成因,其他3个样点的主要属于岩浆来源。剔除了非岩浆来源的数据后的δ-Δ图解法判断CO_2-CH_4间碳同位素分馏达到了平衡。3个样点的CO_2、CH_4碳气体源区温度分别为425~475℃、941~995℃和1179~1578℃。结合最上部地壳温度场结果,我们认为,宁洱火山区现今存在2个壳内岩浆房,分别位于宁洱火山以南和通关火山以北,宁洱岩浆房的温度为1179~1578℃,通关岩浆房的温度为941~995℃。2个岩浆房的现今温度已达到流纹岩浆(600~900℃)、安山岩(800~1100℃)和玄武岩浆(1000~1250℃)的形成温度。思普地震带空间上密集的6级地震丛集活动可以用宁洱岩浆房的高活动性来解释。δ-Δ图解法判断CO_2-CH_4间碳同位素分馏平衡准则应修正为:在保持两拟合直线的斜率符号相反的条件下,δ~(13)CCO_2-ΔCO_2-CH_4拟合直线和δ~(13)CCH_4-ΔCO_2-CH_4拟合直线应相交于δ轴附近截距差Δb≤0.16处。 相似文献
6.
西藏亚东-谷露裂谷带是新生代的活动构造带,具有构造活跃、地震频繁、热泉广布、大地热流高等特征,孕育了丰富的地热资源。已实现商业开发多年的羊八井地热田和羊易地热田正是位于亚东-谷露裂谷带的中部,而位于该构造带北部的谷露地热田地热资源前景和勘探方向还有待深入认识。为此,本文解析了地表地热构造,对比了羊八井地热模式,分析了谷露地热田的深部热动力学背景,并结合钻井试采资料揭示谷露地热田具有良好的地热资源前景。在此基础上,利用大地电磁和重力预测了谷露地热田的地热分布具有南北分带性,即北部和中部具有深部和浅部两个层次的地热储层,而南部地热储层则以浅部为主。为深入研究亚东-谷露裂谷带的地热系统模式及指导地热勘探开发提供了重要的地球物理依据。 相似文献
7.
中国大陆新生代典型火山区温室气体释放的规模及其成因 总被引：5，自引：5，他引：0
火山活动能够将地球深部的碳输送到大气圈,是地质碳排放和深部碳循环的重要形式.火山作用不仅在喷发期能够释放大量温室气体,而且在休眠期也能释放巨量的温室气体.在全球变暖的背景下,定量化地研究火山活动对大气圈温室气体含量增加的贡献具有至关重要的意义.本文利用密闭气室法等该领域国际先进的测试技术,测量并计算了长白山、腾冲、五大连池及青藏高原南部的羊八井等典型火山区的温室气体释放规模.结果显示,我国大陆新生代典型火山区向大气圈输送的温室气体总通量约为8.13×106t·a-1,接近107t·a-1级别,相当于全球火山活动导致的温室气体(主要为CO2)释放总量的6%左右.太平洋构造域火山区的温室气体在释放通量与总量方面均低于特提斯构造域,并且太平洋构造域火山气体的地壳混染程度较低,显示出大洋俯冲带与大陆俯冲带火山区温室气体释放的成因差异. 相似文献
8.
《矿物岩石地球化学通报》2017,(2)
国内外大量研究表明,当今大气圈温室气体浓度的增加是自然因素和人类活动共同作用的结果。地质源温室气体释放是导致当前大气圈温室气体浓度增加的重要自然因素之一。火山-地热区、泥火山系统与油气盆地、巨型活动断裂带等是地质源温室气体的主要释放类型。在当前强调温室气体减排的国际背景下,定量化地评估地质源(主要包括火山-地热区、泥火山系统与油气盆地、巨型活动断裂带等)的温室气体释放通量,对于深入了解人类活动与大气圈温室气体浓度变化的联系至关重要。本文基于中国大陆重要的地质源(主要包括火山-地热区、泥火山系统与油气盆地、巨型活动断裂带等)温室气体的释放特点,重点综述了中国新生代火山-地热区温室气体释放通量与成因研究的近期成果,并进一步讨论了火山-地热区温室气体成分与释放通量的连续观测在中国活火山监测与减灾防灾研究中的应用前景。 相似文献
9.
腾冲新生代火山区CO2气体释放通量及其成因 总被引：2，自引：2，他引：0
许多研究结果表明,休眠期火山主要通过喷气孔、温泉以及土壤微渗漏三种方式向大气圈释放温室气体。腾冲是我国重要的新生代火山区之一,同时也是主要的水热活动区,但是关于温室气体释放通量的研究却鲜有报道。本文首次估算了该地区土壤微渗漏和温泉水的CO2释放通量,并根据气体成分的分析结果探讨了这些温室气体的来源。2012~2013年连续两年使用密闭气室法现场测量了土壤微渗漏CO2通量,结果表明,马站、热海-黄瓜箐和五合-蒲川-团田三个地区通量较高,其中,热海-黄瓜箐地区平均通量最高,马站次之,五合-蒲川-团田地区最低。较高的土壤微渗漏CO2释放地区同前人推断的岩浆囊的分布在空间上具有较好的一致性;三个地区气体的3He/4He比值较高,三端元模拟结果表明,它们均有较高含量的幔源He释放;根据气体CO2/3He与δ13CCO,CO2模拟计算,CO2主要来源于碳酸盐矿物的脱碳作用和岩浆脱气。由此推断2的释放同深部的岩浆囊具有重要的成因联系,它为碳酸盐矿物的脱碳作用提供了主要的热源,同时也是重要的物质来源。根据土壤微渗漏CO2平均通量及火山、地热异常区的分布面积估算出三个地区土壤微渗漏CO2的释放通量分别为1.8×106t/a(马站),3.2×106t/a(热海-黄瓜箐)和2.0×106t/a(五合-蒲川-团田)。腾冲新生代火山区每年通过土壤微渗漏向大气圈释放CO2的量至少可达7.0×106t,为意大利Etna火山区释放CO2通量(1.4×107t/a)的二分之一。通过水岩相互作用计算温泉水中CO2气体的释放通量为4.9×104t/a。腾冲温泉气泡及温泉水向大气圈释放CO2气体的总通量为5.3×104t/a,远高于意大利Vulcano火山区温泉释放的CO2总通量(3.7×103t/a)。 相似文献
10.
地热活动是地球脱气的重要形式之一,其过程常伴随大量温室气体排放。选取非火山地热区西藏玛旁雍热田作为研究对象,基于菲克扩散定律对地热田区土壤CO_2脱气量进行评估。结果表明:该区一般土壤CO_2脱气通量为0.167~0.771 kg/(m2·a),含喷气孔区域土壤CO_2脱气通量为2.054~7.877 kg/(m2·a),含喷气孔地区的土壤CO_2脱气通量是一般土壤脱气量的18.9倍;与全球火山区土壤脱气量(0.001~2.25 Mt/(m2·a))相比,其值显著偏低;但比青藏高原高寒草原生态系统土壤的CO_2排放量(187.46 g/(m2·a))大。结合区域地质背景推测地热系统中的CO_2含量主要来源于岩浆脱气和热液同长石等围岩矿物的蚀变反应。区内土壤CO_2的低脱气通量受透水性较差的碎屑岩沉积盖层约束。 相似文献
11.
Stefan Gödeke Helmut Geistlinger Anko Fischer Hans-Hermann Richnow Mario Schirmer 《Environmental Geology》2008,55(6):1255-1261
Reactive tracer tests are performed to derive flow, transport and in situ biodegradation parameters. This paper describes
the 3D simulation of a reactive tracer test using the transition probability geostatistical approach. Fifty different equally
probable aquifer realizations were generated based on the geological information of 107 boreholes in an area of 62,500 m2. One realization was chosen for the reactive transport simulation based on the results of groundwater flow modeling and on
particle tracking calculations for the site. Field velocities at the site vary between 0.4 and 3 m/d. The transport of the
reactive tracers deuterium ring labeled toluene-d5 and fully deuterated toluene-d8 was simulated and first-order biodegradation rates of 0.017 d−1 for toluene-d5 and 0.012 d−1 for toluene-d8 were determined. 相似文献
12.
Carbon dioxide degassing and thermal energy release in the Monte Amiata volcanic-geothermal area (Italy) 总被引：2，自引：0，他引：2
Francesco Frondini Stefano Caliro Carlo Cardellini Giovanni Chiodini Nicola Morgantini 《Applied Geochemistry》2009
The quaternary volcanic complex of Mount Amiata is located in southern Tuscany (Italy) and represents the most recent manifestation of the Tuscan Magmatic Province. The region is characterised by a large thermal anomaly and by the presence of numerous CO2-rich gas emissions and geothermal features, mainly located at the periphery of the volcanic complex. Two geothermal systems are located, at increasing depths, in the carbonate and metamorphic formations beneath the volcanic complex. The shallow volcanic aquifer is separated from the deep geothermal systems by a low permeability unit (Ligurian Unit). A measured CO2 discharge through soils of 1.8 × 109 mol a−1 shows that large amounts of CO2 move from the deep reservoir to the surface. A large range in δ13CTDIC (−21.07 to +3.65) characterises the waters circulating in the aquifers of the region and the mass and isotopic balance of TDIC allows distinguishing a discharge of 0.3 × 109 mol a−1 of deeply sourced CO2 in spring waters. The total natural CO2 discharge (2.1 × 109 mol a−1) is slightly less than minimum CO2 output estimated by an indirect method (2.8 × 109 mol a−1), but present-day release of 5.8 × 109 mol a−1 CO2 from deep geothermal wells may have reduced natural CO2 discharge. The heat transported by groundwater, computed considering the increase in temperature from the infiltration area to the discharge from springs, is of the same order of magnitude, or higher, than the regional conductive heat flow (>200 mW m−2) and reaches extremely high values (up to 2700 mW m−2) in the north-eastern part of the study area. Heat transfer occurs mainly by conductive heating in the volcanic aquifer and by uprising gas and vapor along fault zones and in those areas where low permeability cover is lacking. The comparison of CO2 flux, heat flow and geological setting shows that near surface geology and hydrogeological setting play a central role in determining CO2 degassing and heat transfer patterns. 相似文献
13.
There are many arguments on energy sources and main controlling factors of geothermal fields, so a systematic study on the distribution of ground temperature fields shall be necessary. In this paper the thermal conduction forward method of geothermal field is used to simulate cooling rate of abnormal heat sources and heat transfer of the paleo-uplift model. Combined with a large number of geothermal field exploration cases and oil exploration well temperature curves of domestic and foreign, the following conclusions are drawn:(1) According to the magmatic activity time, the magmatism activities are divided into two categories: Magma active areas(activity time 500 000 years) and weak/magma inactive areas(activity time 500 000 years). The latter has a fast cooling rate(the cooling time of the magma pocket buried around 10 km is less than 200 000 years) after it has intruded into the shallow layer and it has no direct contribution to modern geothermal fields;(2) China belongs to a weak/magma inactive area such as Tengchong region and Qinghai-Tibet region because the chronological data of these regions show that its magma activity time is more than 500 000 years;(3) The temperature of most geothermal fields can be obviously divided into three segments in the vertical direction: A high geothermal gradient segment(Segment H) at the surface, then a low geothermal gradient segment(Segment L) at a secondary depth, and finally a lower temperature segment(Segment D) at a deeper depth. The temperature isoline presents a mirror reflection relation on the temperature profile, indicating that geothermal field is dominated by heat conduction, rather than having an abnormally high temperature "heat source" to provide heat;(4) Near-surface(0-5 km) materials' lateral heterogeneity caused by tectonic movement shall probably be the main controlling factor of ground temperature fields. 相似文献
14.
There are many arguments on energy sources and main controlling factors of geothermal fields, so a systematic study on the distribution of ground temperature fields shall be necessary. In this paper the thermal conduction forward method of geothermal field is used to simulate cooling rate of abnormal heat sources and heat transfer of the paleo-uplift model. Combined with a large number of geothermal field exploration cases and oil exploration well temperature curves of domestic and foreign, the following conclusions are drawn: (1) According to the magmatic activity time, the magmatism activities are divided into two categories: Magma active areas (activity time < 500 000 years) and weak/magma inactive areas (activity time > 500 000 years). The latter has a fast cooling rate (the cooling time of the magma pocket buried around 10 km is less than 200 000 years) after it has intruded into the shallow layer and it has no direct contribution to modern geothermal fields; (2) China belongs to a weak/magma inactive area such as Tengchong region and Qinghai-Tibet region because the chronological data of these regions show that its magma activity time is more than 500 000 years; (3) The temperature of most geothermal fields can be obviously divided into three segments in the vertical direction: A high geothermal gradient segment (Segment H) at the surface, then a low geothermal gradient segment (Segment L) at a secondary depth, and finally a lower temperature segment (Segment D) at a deeper depth. The temperature isoline presents a mirror reflection relation on the temperature profile, indicating that geothermal field is dominated by heat conduction, rather than having an abnormally high temperature “heat source” to provide heat; (4) Near-surface (0-5 km) materials’ lateral heterogeneity caused by tectonic movement shall probably be the main controlling factor of ground temperature fields. 相似文献
15.
The effect of the curvature of open magnetic field lines on the generation of electric fields in radio pulsars is considered in the framework of a Goldreich-Julian model, for both a regime with a free outflow of electrons from the neutron-star surface and the case of a small thermoemission current. An expression for the electron thermoemission current in a strong magnetic field is derived. The electric field associated with the curvature of the magnetic flux tubes is comparable to the field generated by the relativistic dragging of the inertial frames. 相似文献
16.
V.G. Zolotarev 《Journal of Geochemical Exploration》1984,21(1-3)
The concentration of metals and ores in thermal fields of intrusive bodies can be analyzed by numerical simulation (modelling) of the heat-mass transfer process. A knowledge of the dynamics and the movement of the temperature and crystallization fronts, as well as an understanding of the characteristics of the thermal gradients, heat flows, energy, and thermal stresses which result in the formation of fracture zones, are necessary for an estimation of the spacial and temporal aspects of the mass balance calculations and the ore concentration processes. The application of the method is illustrated by observing the changes in the rare earth element concentration in a vein-type apatite orebody in limestone which has been intruded by a post-ore dike. The method has potential value in exploring for hidden mineralization. 相似文献
17.
A methodology for the anisotropic characterization of macroseismic fields is proposed, in order to evaluate seismic hazard, based on the real geometry of the isoseismals of the field. The proposed methodology, independent of the macroseismic intensity attenuation law, allows both for a single field and for several fields in the same source zone, the determination of minimum and maximum attenuation values and of the relative directions. 相似文献
18.
19.
The mechanism of magnetodipole braking of radio pulsars is used to calculate new values of the surface magnetic fields of neutron stars. The angles β between the spin axes and magnetic moments of the neutron stars were estimated for 376 radio pulsars using three different methods. It is shown that small inclinations of magnetic axes dominate. The equatorial magnetic fields for the considered sample of pulsars are calculated using the β values obtained. As a rule, these magnetic fields are a factor of a few higher than the corresponding values in known catalogs. 相似文献
20.