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1.
Natural gas hydrate contains a specific amount of heavy hydrocarbons, such as ethane, propane, etc., aside from the primary guest gas of methane. Although the coexistence of two or even three hydrate structures has been discovered at several hydrate sites, the requisite formation mechanism is still not well understood. In-situ observation of the formation process of mixed methane-propane hydrate in a confined space was conducted using confocal Raman imaging microscopy. The Raman imaging results reveal that sI methane hydrate and sII mixed methane-propane hydrate are formed and coexist in the reaction system. In the confined space, the sI hydrate originates from the dissolved gas in water, while the sII hydrate is formed from free gas. The results obtained can help explain the coexistence of sI and sII hydrates found in natural hydrate samples, as well as providing insights into a possible dynamic scenario of hydrate reservoirs in geological history. 相似文献
2.
Most submarine gas hydrates are located within the two-phase equilibrium region of hydrate and interstitial water with pressures (P) ranging from 8 to 60 MPa and temperatures (T) from 275 to 293 K. However, current measurements of solubilities of methane in equilibrium with hydrate in the absence of a vapor phase are limited below 20 MPa and 283.15 K, and the differences among these data are up to 30%. When these data were extrapolated to other P-T conditions, it leads to large and poorly known uncertainties. In this study, in situ Raman spectroscopy was used to measure methane concentrations in pure water in equilibrium with sI (structure one) methane hydrate, in the absence of a vapor phase, at temperatures from 276.6 to 294.6 (±0.3) K and pressures at 10, 20, 30 and 40 (±0.4%) MPa. The relationship among concentration of methane in water in equilibrium with hydrate, in mole fraction [X(CH4)], the temperature in K, and pressure in MPa was derived as: X(CH4) = exp [11.0464 + 0.023267 P − (4886.0 + 8.0158 P)/T]. Both the standard enthalpy and entropy of hydrate dissolution at the studied T-P conditions increase slightly with increasing pressure, ranging from 41.29 to 43.29 kJ/mol and from 0.1272 to 0.1330 kJ/K · mol, respectively. When compared with traditional sampling and analytical methods, the advantages of our method include: (1) the use of in situ Raman signals for methane concentration measurements eliminates possible uncertainty caused by sampling and ex situ analysis, (2) it is simple and efficient, and (3) high-pressure data can be obtained safely. 相似文献
3.
热液金刚石压腔 (HDAC)在地质上的应用及甲烷水合物合成实验研究 总被引：16，自引：4，他引：12
热液金刚石压腔 (HDAC)是 2 0世纪末发展起来的一种高温高压及低温高压实验技术。它可在 - 180～ 12 0 0℃ ,10 0～ 10 0 0 0MPa水热体系进行实验 ,并具直观实验全过程的特点。文中首次运用HDAC在水体系中对哀牢山花岗岩进行了熔融实验 ,在显微镜下观察到花岗岩熔融过程 ,其初熔温度为 712 88～ 714 87℃ ,压力为 2 2 5MPa ,熔融温度为 759 54～76 0 0 0℃ ,压力为 30 0MPa。重点介绍了国外运用HDAC进行冰的高压相、水体系中伟晶岩矿物溶解、可燃有机岩、石油及岩石热解、高压下矿物包裹体均一温度测定及甲烷水合物合成实验研究新成果。甲烷水合物在永久冻土带及大陆坡、海底高原、海底沉积物等地质环境广泛分布 ,储量大 ,可成为 2 1世纪人类使用的新能源。目前世界主要国家的科学家除致力于该资源勘探外 ,还运用不同方法进行甲烷水合物的合成研究 ,以了解其形成条件及性质。开发和应用甲烷水合物具有重大意义 ,为促进我国此项工作开展 ,文中作了重点介绍。 相似文献
4.
自然地质条件下不同气源的天然气体由于其组成不同,对天然气水合物的成藏条件产生不同影响。以2个常规天然气样品为例,在中国石油大学自行研制的水合物成藏一维模拟实验装置上进行了水合物成藏模拟实验,并对实验前后的原始气样、水合物形成后的游离气、分解气进行了气体组分分析。实验结果表明：水合物分解气中CH4、N2含量降低,而C2H6、C3H8、iC4H10、nC4H10、CO2含量增大,游离气中各组分的变化趋势刚好相反,这意味着同等的温度压力条件下,C2H6、C3H8、iC4H10、nC4H10、CO2等与CH4、N2相比更易于形成水合物;通过计算分解气体各组分相对于原始气体的相对变化量发现,在实验温度压力条件下（高压釜温度范围为4~10 ℃,气体进口压力为5 MPa）,烃类气体与水结合形成水合物的能力由甲烷、乙烷、丙烷、异丁烷依次增加;由于不同烃类气体与水合物结合的条件不同,导致水合物形成过程中气体组分发生分异,水合物中甲烷含量减少、湿气含量增大,而游离气中气体变化相反,在自然地质条件下形成由水合物稳定带上部溶解气带、水合物稳定带及下部游离气带（或常规气藏）甲烷含量呈中-低-高特点,湿气和二氧化碳含量呈低-高-中的三层结构分布模式,因此,同一气源气体在不同带内表现出不同的气体组分特征。 相似文献
5.
《China Geology》2020,3(3):362-368
Gas hydrate is one kind of potential energy resources that is buried under deep seafloor or frozen areas. The first trial offshore production from the silty reservoir was conducted in the South China Sea by the China Geological Survey (CGS). During this test, there were many unique characteristics different from the sand reservoir, which was believed to be related to the clayed silt physical properties. In this paper, simulation experiments, facilities analysis, and theoretical calculation were used to confirm the hydrate structure, reservoir thermo-physical property, and bond water movement rule. And the behavior of how they affected production efficiency was analyzed. The results showed that: It was reasonable to use the structure I rather than structure II methane hydrate phase equilibrium data to make the production plan; the dissociation heat absorbed by hydrate was large enough to cause hydrate self-protection or reformation depend on the reservoir thermal transfer and gas supply; clayed silt got better thermal conductivity compared to coarse grain, but poor thermal convection especially with hydrate; clayed silt sediment was easy to bond water, but the irreducible water can be exchanged to free water under high production pressure, and the most obvious pressure range of water increment was 1.9–4.9 MPa. 相似文献
6.
在定容条件下,实验研究了甲烷水合物在含水量不同的多孔海泥中的生成特性。所使用的海泥平均孔径为12178 nm,总孔容为4997×10-2 ml/g,比表面积为16412 m2/g。所用海泥样品含水量为40%,实验的温度范围为27415~28115 K,初始生成压力范围为102~144 MPa。实验结果表明,甲烷水合物在海泥中的生成速率以及气体消耗量随着初始压力的增加而增大,随着温度的降低而增大。海泥的复杂孔隙结构能够促进水合物的成核,但会降低水的最终转化率,其作用随着温度的升高与压力的降低而增大。 相似文献
7.
We present here a thermodynamic model for predicting multi-phase equilibrium of methane hydrate liquid and vapor phases under conditions of different temperature,pressure,salinity and pore sizes.The model is based on the 1959 van der Waals—Platteeuw model,angle-dependent ab initio intermolecular potentials,the DMW-92 equation of state and Pitzer theory.Comparison with all available experimental data shows that this model can accurately predict the effects of temperature,pressure, salinity and capillary r... 相似文献
8.
甲烷水合物在AlCl3溶液中的相平衡条件 总被引：1，自引：0，他引：1
利用可视法测定了甲烷水合物在AlCl3溶液中的三相平衡(甲烷水合物-AlCl3液相-甲烷气相)条件.AlCl3溶液中甲烷水合物的生成压力为4.040～8.382 MPa,温度为272.15～278.15 MPa.对相同摩尔浓度的AlCl3和KCl溶液中甲烷水合物生成条件的抑制作用进行了讨论.并将实验结果与前人的研究数据进行了对比,通过统计分析得到一计算甲烷水合物相平衡压力与温度的经验公式,经计算所得结果与实验数据一致.研究认为AlCl3溶液可以作为一种良好的抑制剂用于油气工业的输送管道中。 相似文献
9.
The Shenhu gas hydrate drilling area is located in the central Baiyun sag, Zhu Ⅱ depression, Pearl River Mouth basin, northern South China Sea. The gas compositions contained in the hydrate-bearing zones is dominated by methane with content up to 99.89% and 99.91%. The carbon isotope of the methane (δ13C1 ) are 56.7‰ and 60.9‰, and its hydrogen isotope (δD) are 199‰ and 180‰, respectively, indicating the methane from the microbial reduction of CO2 . Based on the data of measured seafloor temperature and geothermal gradient, the gas formed hydrate reservoirs are from depths 24-1699 m below the seafloor, and main gas-generation zone is present at the depth interval of 416-1165 m. Gas-bearing zones include the Hanjiang Formation, Yuehai Formation, Wanshan Formation and Quaternary sediments. We infer that the microbial gas migrated laterally or vertically along faults (especially interlayer faults), slump structures, small-scale diapiric structures, regional sand beds and sedimentary boundaries to the hydrate stability zone, and formed natural gas hydrates in the upper Yuehai Formation and lower Wanshan Formation, probably with contribution of a little thermogenic gas from the deep sedments during this process. 相似文献
10.
Oceanic gas hydrates have been measured near the seafloor for the first time using a seagoing Raman spectrometer at Hydrate Ridge, Oregon, where extensive layers of hydrates have been found to occur near the seafloor. All of the hydrates analyzed were liberated from the upper meter of the sediment column near active gas venting sites in water depths of 770-780 m. Hydrate properties, such as structure and composition, were measured with significantly less disturbance to the sample than would be realized with core recovery. The natural hydrates measured were sI, with methane as the predominant guest component, and minor/trace amounts of hydrogen sulfide present in three of the twelve samples measured. Methane large-to-small cage occupancy ratios of the hydrates varied from 1.01 to 1.30, in good agreement with measurements of laboratory synthesized and recovered natural hydrates. Although the samples visually appeared to be solid, varying quantities of free methane gas were detected, indicating the possible presence of occluded gas in a hydrate bubble fabric. 相似文献
11.
多步分解法初步研究石英砂中甲烷水合物p-T稳定条件 总被引：1，自引：0，他引：1
设计加工了一套研究海底沉积物水合物稳定条件实验装置,采用多步加热分解的方法对不同孔隙度的石英砂沉积物甲烷水合物相态平衡点(p-T稳定条件)进行了初步研究。为校验实验装置和实验方法,首先对甲烷水合物在十二烷基硫酸钠(SDS)溶液中的生成和分解过程进行了研究,获得的实验数据与文献数据吻合得很好。在此基础上,以4种不同粒径(96~180μm、180~380μm、212~380μm和380~830μm)的石英砂为介质,分别研究了甲烷水合物的p-T稳定条件。结果表明,实验测得的数据与纯水溶液中的结果基本一致,说明在实验所用的不同粒径石英砂构成的孔隙尺度内,毛细管作用对水合物相态点的影响可以忽略。 相似文献
12.
Overview of the MITI Nankai Trough Wells: A Milestone in the Evaluation of Methane Hydrate Resources 总被引：4，自引：0，他引：4
Yoshihiro Tsuji Hisashi Ishida Masaru Nakamizu Ryo Matsumoto Satoshi Shimizu 《Resource Geology》2004,54(1):3-10
Abstract. Bottom-simulating reflectors suggestive of the presence of methane hydrates are widely distributed below the ocean floor around Japan. In late 1999, drilling of the MITI Nankai Trough wells was conducted to explore this potential methane hydrate resource and a Tertiary conventional structure. The wells are located in the Northwest Pacific Ocean off Central Japan at a water depth of 945 m. A total of six wells were drilled, including the main well, two pilot wells, and three post survey wells at intervals of 10–100 m. All wells except the first confirmed the occurrence of hydrates based on logging-while-drilling, wire-line logging and/or coring using a pressure and temperature coring system in addition to conventional methods. Based on the various well profiles, four methane hydrate-bearing sand-rich intervals in turbidite fan deposits were recognized. Methane hydrates fill the pore spaces in these deposits, reaching saturation of up to 80 % in some layers. The methane hydrate-bearing turbiditic sand layers are less than 1 m thick, with a total thickness of 12–14 m. The bottom depth of high hydrate concentration correlates well with the depth of the bottom-simulating reflector. Based on these exploration results, the Japanese government inaugurated a 16-year methane hydrate exploitation program in 2001. 相似文献
13.
14.
JIN Chunshuang WANG JiyangInstitute of Geology Geophysics Chinese Academy of Sciences Beijing Strategic Research Center for Oil Gas Resources Ministry of Land Resources Beijing 《《地质学报》英文版》2002,76(4):423-428
Based on the analysis of sea-bottom temperature and geothermal gradient, and by means of the phase boundary curve of gas hydrate and the sea-bottom temperature versus water depth curve in the South China Sea, this paper studies the temperature and pressure conditions for gas hydrate to keep stable. In a marine environment, methane hydrate keeps stable at water depths greater than 550 m in the South China Sea. Further, the thickness of the gas hydrate stability zone in the South China Sea was calculated by using the phase boundary curve and temperature-depth equations. The result shows that gas hydrate have a better perspective in the southeast of the Dongsha Islands, the northeast of the Xisha Islands and the north of the Nansha Islands for thicker stability zones. 相似文献
15.
天然气水合物粉晶X射线衍射测试参数优化及分析方法 总被引：1，自引：1，他引：0
天然气水合物是由烃类气体和水在低温高压下形成的一种非化学计量的笼型晶体水合物,在常温常压下极易分解,需要在低温条件下对其进行测试。本文针对天然气水合物这一特殊样品,重点研究其粉晶X射线衍射测试条件,系统地探讨了步长、扫描速度、累加次数及测试温度等因素对测试结果的影响,优化了仪器参数,建立了粉晶X射线衍射测试天然气水合物晶体结构的方法,并应用到实验合成的甲烷水合物和我国南海珠江口盆地钻获的天然气水合物样品的晶体结构测试中。结果表明,我国南海珠江口盆地的天然气水合物样品与实验合成的甲烷水合物结构相同,均属立方晶系,为典型的Ⅰ型水合物,晶胞参数分别为11.9309×10~(-10)m和11.9135×10~(-10)m。该技术可准确获得天然气水合物的结构信息,为我国天然气水合物的深入研究提供技术支撑。 相似文献
16.
海底多相流动区域沉积物孔隙内流体迁移-甲烷输运-水合物形成是一种普遍模式,形成的水合物在孔隙内沉淀并与多孔介质骨架胶结从而改变当地的地层结构和性质。水合物的不断形成将减少沉积地层孔隙度,改变孔隙内各相间界面张力,增大当地孔隙的进入压力及毛细压力,增强地层滞后效应,降低地层渗透率,同时多相流体流动前缘气液分离带变厚而使得气柱变长。建立了在这类环境里水合物-水-气-盐共同作用下的水合物成藏模型,选择合适的参数分析了水合物形成对沉积地层静水力学性质等的影响关系。最后根据资料估算了南海北部神狐海域沉积物内甲烷气柱的分布,结果表明：随着水合物在沉积物孔隙内逐渐饱和,临界甲烷气柱长度将在接近海底面处达到最大,约为09 m。 相似文献
17.
Shin-Ichi Machida Hisako Hirai Taro Kawamura Yoshitaka Yamamoto Takehiko Yagi 《Physics and Chemistry of Minerals》2007,34(1):31-35
High-pressure Raman studies of methane hydrate were performed using a diamond anvil cell in the pressure range of 0.1–86 GPa
at room temperature. Raman spectra of the methane molecules revealed that new softened intramolecular vibration mode of ν
1 appeared at 17 GPa and that the splitting of vibration mode of ν
3 occurred at 15 GPa. The appearance of these two modes indicates that an intermolecular attractive interaction increases between
the methane molecules and the host water molecules and between the neighboring methane molecules. These interactions might
result in the exceptional stability of a high-pressure structure, a filled ice Ih structure (FIIhS) for methane hydrate, up
to 40 GPa. At 40 GPa, a clear change in the slope of the Raman shift versus pressure occurred, and above 40 GPa the Raman
shift of the vibration modes increased monotonously up to 86 GPa. A previous XRD study showed that the FIIhS transformed into
another new high-pressure structure at 40 GPa. The change in the Raman spectra at 40 GPa may be induced by the transition
of the structure. 相似文献
18.
现代暖期(Current Warm Period,CWP,1850—至今)以来全球气温升高,南海北部陆坡底层海水温度升高、海平面上升影响海底天然气水合物稳定性。为探究现代暖期气候变暖对南海北部陆坡水合物分解影响,本文模拟计算了东沙海域、神狐海域、西沙海域、琼东南海域水合物赋存水深最浅处水合物的饱和度在1 000年内变化情况,评估了受现代暖期气候变暖影响水合物赋存水深范围,讨论了水合物分解量及其对环境影响。结果发现:(1)受现代暖期气候变暖影响,东沙海域、西沙海域、琼东南海域水合物分解,神狐海域水合物不分解;当东沙海域、西沙海域、琼东南海域水深分别超过665、770、725 m,水合物不分解;(2)现代暖期自始以来,南海北部陆坡水合物分解量为9.36×107~3.83×108 m3,产生的甲烷量为1.54×1010~6.28×1010 m3;(3)受现代暖期气候变暖影响,南海北部陆坡每年水合物分解量为5.5×105~2.25×106 m3,产生的甲烷量为9.02×107~3.69×108 m3,这些甲烷中3.61×105~1.48×106 m3能够进入大气,对温室效应贡献度为每年我国人类生活的0.01%~0.06%;与此同时,1.77×107~7.23×107 m3甲烷可能会在海水中被氧化形成弱酸,加重南海北部陆坡海水酸化。 相似文献
19.
煤的吸附能力是决定煤层含气量大小和煤层气开发潜力的重要储层参数。通过对沁南-夏店区块二叠系山西组3号煤层72个煤样进行等温吸附实验,剖析了3号煤层煤的吸附性能,建立了基于Langmuir方程的煤层含气量预测方法,揭示了研究区3号煤层煤的吸附性能及含气量分布。研究结果表明,沁南-夏店区块3号煤层主要为贫煤和无烟煤,煤的空气干燥基Langmuir体积为18.15~34.75 m3/t,平均29.36 m3/t;Langmuir压力为1.47~2.71 MPa,平均2.03 MPa;煤储层压力梯度0.11~1.06 MPa/hm,平均0.49 MPa/hm,煤储层压力随着煤层埋藏深度的增加而增高;煤层含气饱和度整体呈欠饱和状态。通过预测模型预测研究区3号煤层含气量2.87~24.63 m3/t,平均13.78 m3/t,且随着埋藏深度的增加而增高,其含气量相对沁水盆地南部偏低。煤储层含气量分布主要受控于本区煤层生气、储气和保存等因素。 相似文献
20.
对不同温度（90~200 ℃）和压力（20~120 MPa）条件下的富甲烷天然气在碳酸氢钠溶液中的溶解度值进行了实验测定,阐述了甲烷溶解度随温度、压力及矿化度的变化特征。综合前人的实验结果,将天然气的溶解度与温度的关系划分为3个阶段: ①缓慢递减阶段（0~80 ℃）;②快速递增阶段（>80~150 ℃）;③缓慢递增阶段（>150 ℃）。在温压的共同作用下,溶解度随埋藏深度的增加,也具有不同的阶段变化特征;且当地层水温度、压力足够高时,甲烷的溶解能力趋近于某一极限值。利用甲烷溶解度回归方程有助于对不同地区水溶气析离脱气界限的估算。我国主要存在包括侧向阶段脱气、断裂-底辟脱气、盖层渗滤脱气和构造抬升脱气4种与构造和渗滤作用有关的水溶气析离成藏模式。 相似文献