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1.
To understand the origin of the methane distributions in sediments of Eckernförde Bay, three sites were sampled in May 1994 for determination of methane, sulfate and chloride concentrations in the sediment porewaters. In much of the Bay, bubbles of biogenic methane gas within the sediments lead to widespread ‘acoustic turbidity’ seen in acoustic surveys, masking the sedimentary structure below the gassy horizon. Acoustic windows, where the gas does not appear to be present, occur in several locations in the Bay, often surrounded by acoustically turbid sediments. Pockmarks, shallow depressions in the sediment, are also found in Bay sediments and may show acoustic turbidity at even shallower depths below the interface than surrounding sediments. One site of each type was sampled in this study. The site probably representative of much of the bay below 20 m water depth, revealed methane saturated conditions by about 75 cm depth below the interface, confirming inferences from acoustic scattering data that free gas was present in the sediment. Above this, the methane concentration profile was concave-upward, indicative of methane oxidation in the overlying, sulfate-reducing sediments. These porewaters showed a slightly decreasing chlorinity with depth. At an acoustic window site, methane concentrations rose to a maximum at about 125 cm depth, but did not reach saturation. Below this depth they decreased in a concave-down pattern. Chloride concentrations decreased markedly with depth, indicative of vertical freshwater flow from below. The third site was a pockmark exhibiting very shallow acoustic turbidity at about 25 cm depth. Here methane concentrations rose to exceed saturation within 25 cm depth below the interface and the porewaters became almost fresh by 1.5 m depth, indicative of a stronger flow of freshwater from below. These groundwater flows have competing effects on the methane inventory. They help exclude sulfate from the sediment, allowing the earlier/shallower onset of methanogenesis, but they also aid loss of methane through advection. A diagenetic model that couples the biogeochemistry of sulfate and methane is used to explain the presence or absence of methane gas in these sediments in relation to the flow rate of fresh groundwater from below. Model results indicate that acoustic windows within otherwise acoustically turbid sediments of the bay are likely due to relatively higher rates of vertical advection of fresh groundwater. The gassy pockmark, however, with an even higher vertical advection rate, seems to require the input of additional reactive organic carbon to explain its vertical methane distribution. 相似文献
2.
除合适的温度和压力条件外,甲烷水合物的形成还需要有充足的甲烷供给,沉积物孔隙水中的甲烷浓度必须大于甲烷水合物的溶解度.本文建立了水合物－水－游离气三相体系、水合物－水二相体系、气－水二相体系的甲烷溶解度计算优选方法,计算确定了水合物系统的甲烷溶解度-深度相图,依此划分出游离气、溶解气、水-水合物、水-水合物-游离气四个甲烷不同相态分布区.对水合物脊ODP1249和1250钻位、布莱克海台ODP997钻位稳定带甲烷水合物含量和稳定带之下游离气含量进行了计算.ODP1249浅部13.5～72.4 mbsf(mbsf表示海底以下深度)的甲烷水合物是沉积物孔隙体积的10%～61%,ODP1250钻位35～1065 mbsf的甲烷水合物约为孔隙体积的0.7%～1.9%,水合物层之下游离气层厚约22 m,游离气含量约占孔隙的4%.布莱克海台ODP997钻位的浅部146.9 mbsf处无水合物发育,202.4～433.3 mbsf之间水合物占孔隙体积的约5%～7%,水合物层之下游离气层厚约80 m,游离甲烷含量为孔隙的0.2%～28%. 相似文献
3.
近年来,活动冷泉的研究越来越受到关注.本文利用多波束数据、多道地震数据以及底质取样结果研究琼东南海域活动冷泉系统,分析活动冷泉的羽状流特征、海底地貌与底质特征以及流体活动构造特征.多波束水体数据上,观测到多个延伸高度超过750 m的气泡羽状流,海底流体活动非常强烈;多道地震上识别出麻坑、流体运移通道、气烟囱等流体渗漏相关的构造,与其他海域观测到的反射特征不同,羽状流的下方流体运移通道呈强振幅"串珠"反射;重力活塞取样在两个站位上获得浅表层块状天然气水合物.其中一个站位位于活动冷泉附近,天然气水合物赋存于海底以下8 m左右.基于以上三方面的数据,笔者提出了一个用于描述活动冷泉系统的形成模式,游离气通过气烟囱向上运移到达浅层,一部分在天然气水合物稳定带内形成天然气水合物,另一部分穿透天然气水合物稳定带到达海底,形成活动冷泉的羽状流. 相似文献
4.
海洋环境中天然气水合物层是理想的毛细管封闭层,游离气被抑制在水合物层下,游离气层的气体压力随气体聚集和气层厚度的增加而升高,当气压超过封闭层的毛细管力时,游离气会克服毛细管进入压力、刺入上伏封闭层孔隙空间,毛细管封闭作用随之消失,从而形成水合物下伏游离气向海底的渗漏.通过对该过程进行的数值模拟计算表明：渗漏气体是以活塞式驱动上伏沉积层中的孔隙水向海底排出,水合物稳定带内流体渗漏速度随水流柱高度的减小而增加,当水流阻抗大于相应沉积层段的静岩压力时,沉积层将转变为流沙,流沙沉积被海流移除后便在海底留下凹陷麻坑.麻坑形成后流体运移通道演化为气体通道,气体快速排放.麻坑深度主要取决于游离气层的厚度和水合物封闭层（底界）的深度,而与沉积层的渗透率无关.麻坑深度一定程度上指示了渗漏前水合物层下伏游离气层的资源量.对布莱克海台海底麻坑深度的数值模拟计算表明,形成4 m深的海底麻坑需要至少22 m厚的游离气层. 相似文献
5.
天然气水合物体系动态演化研究(Ⅱ):海底滑坡 总被引：2，自引：5，他引：2
天然气水合物被认为是大陆边缘沉积物强度变弱的一个因子，从而能解释大陆边缘海底滑坡的一些观测现象。天然气水合物的形成使沉积物强度增加，而其分解则使沉积物强度变弱。虽然无法直接观测沉积物中天然气水合物的活动过程与相应的海底滑坡，大量的背景资料表明，天然气水合物崩解常常有助于触发海底沉积物块体的运动。此外，大型滑塌可以释放大量的固态天然气水合物，水合物在水柱中上浮。大块天然气水合物可以在分解前到达海洋的上部层，一些甲烷可以直接进入大气中。本文综述与天然气水合物体系演化有关的海底滑坡的研究现状。 相似文献
6.
《Earth and Planetary Science Letters》2006,241(1-2):211-226
We present an equilibrium model of methane venting through the hydrate stability zone at southern Hydrate Ridge, offshore Oregon. Free gas supplied from below forms hydrate, depletes water, and elevates salinity until pore water is too saline for further hydrate formation. This system self-generates local three-phase equilibrium and allows free gas migration to the seafloor. Log and core data from Ocean Drilling Program (ODP) Site 1249 show that from the seafloor to 50 m below seafloor (mbsf), pore water salinity is elevated to the point where liquid water, hydrate and free gas coexist. The elevated pore water salinity provides a mechanism for vertical migration of free gas through the regional hydrate stability zone (RHSZ). This process may drive gas venting through hydrate stability zones around the world. Significant amount of gaseous methane can bypass the RHSZ by shifting local thermodynamic conditions. 相似文献
7.
Improved estimates of the amount of subsurface gas hydrates are needed for natural resource, geohazard, and climate impact assessments. To evaluate gas hydrate saturation from seismic methods, the properties of pure gas hydrates need to be known. Whereas the properties of sediments, specifically sands, and hydrate‐bearing sediments are well studied, the properties of pure hydrates are largely unknown. Hence, we present laboratory ultrasonic P‐wave velocity and attenuation measurements on pure tetrahydrofuran hydrates as they form with reducing temperatures from 25°C to 1°C under atmospheric pressure conditions. Tetrahydrofuran hydrates, with structure II symmetry, are considered as proxies for the structure I methane hydrates because both have similar effects on elastic properties of hydrate‐bearing sediments. We find that although velocity increased, the waveform frequency content and amplitude decreased after the hydrate formation reaction was complete, indicating an increase in P‐wave attenuation after hydrate formation. When the tetrahydrofuran hydrate was cooled below the freezing point of water, velocity and quality factor increased. Nuclear Magnetic Resonance results indicate the presence of water in the “pure hydrate” samples above the water freezing point, but none below. The presence of liquid water between hydrate grains most likely causes heightened attenuation in tetrahydrofuran hydrates above the freezing point of water. In naturally occurring hydrates, a similarly high attenuation might relate to the presence of water. 相似文献
8.
琼东南盆地油气地质显示盆地内具有生物成因和热成因天然气的巨大生成能力和远景. 地震剖面显示盆地内发育有泥底辟和气烟囱、沟通泥底辟和气烟囱与海底的断裂及可能正在活动的天然气冷泉,这些特征非常有利于天然气水合物的发育. 通过天然气水合物热力学稳定域预测,确定了琼东南盆地天然气水合物的平面和剖面分布特征. 生物成因甲烷水合物分布于水深大于约600m的海底,稳定带最大厚度约314m;热成因天然气水合物分布于水深大于约450m的海区,稳定带最大厚度约410m. 盆地内天然气水合物远景总量约10×109m3,水合物天然气远景为1.6×1012m3. 相似文献
9.
以三维高分辨地震与海底高频地震仪（OBS）联合勘探数据为基础,获得海底之下沉积层的地震反射成像剖面及多波信息,并以此确定研究区含天然气水合物沉积层的纵、横波速度的变化特征.根据走时反演获得的横波速度与纵波速度对比分析发现,研究区海底之下500 m深度范围内的某些沉积层具有较高的纵横波速度,这一纵波速度升高区域与水合物稳定带对应,而纵波速度下降并且横波速度变化较小的区域,可能与游离气的存在相关.游离气的可能存在与基于这一区域2007年钻探测井结果的普遍认识不完全相符. 相似文献
10.
Acoustic turbidity caused by the presence of gas bubbles in seafloor sediments is a common occurrence worldwide,but is as yet poorly understood. The Coastal Benthic Boundary Layer experiment in the Baltic off northern Germany was planned to better characterize the acoustic response of a bubbly sediment horizon. In this context, in situ measurements of compressional wave speed and attenuation were made over the frequency range of 5–400 kHz in gassy sediments of Eckernförde Bay. Dispersion of compressional speed data was used to determine the upper limit of the frequency of methane bubble resonance at between 20 and 25 kHz. These data, combined with bubble size distributions determined from CT scans of sediments in cores retained at ambient pressure, yield estimates of effective bubble sizes of 0.3–5.0 mm equivalent radius. The highly variable spatial distribution of bubble volume and bubble size distribution is used to reconcile the otherwise contradictory frequency-dependent speed and attenuation data with theory. At acoustic frequencies above resonance (>25 kHz) compressional speed is unaffected by bubbles and scattering from bubbles dominates attenuation. At frequencies below resonance (<1 kHz) ‘compressibility effects’ dominate, speed is much lower (250 m s-1) than bubble-free sediments, and attenuation is dominated by scattering from impedance contrasts. Between 1.5 and 25 kHz bubble resonance greatly affects speed and attenuation. Compressional speed in gassy sediments (1100–1200 m s-1) determined at 5–15 kHz is variable and higher than predicted by theory (<250 m s-1). These higher measured speeds result from two factors: speeds are an average of lower speeds in gassy sediments and higher speeds in bubble-free sediments; and the volume of smaller-sized bubbles which contribute to the lower observed speeds is much lower than total gas volume. The frequency-dependent acoustic propagation is further complicated as the mixture of bubble sizes selectively strips energy near bubble resonance frequencies (very high attenuation) allowing lower and higher frequency energy to propagate. It was also demonstrated that acoustic characterization of gassy sediments can be used to define bubble size distribution and fractional volume. 相似文献
11.
对南海东北部973项目采集的地震测线进行了处理,阐明了恒春海脊处天然气水合物似海底反射（BSR）的特征.不同类型剖面的分析表明,单道地震剖面可以揭示南海东北部地区BSR一定的分布,但地震处理对揭示BSR分布全貌起重要作用.南海东北部的BSR具有世界大陆边缘BSR典型的特征,切穿了沉积层理反射,与海底起伏大体平行,为一强振幅的负极性反射.该BSR特征明显,意味着南海东北部地区存在含天然气水合物沉积.利用甲烷水合物与多组分天然气水合物相平衡曲线,计算了稳定带底界的埋深,并与BSR深度进行了对比分析.无论是甲烷水合物稳定带底界还是多组分天然气水合物稳定带的底界,单一地温梯度计算的结果不可能与BSR深度在整个剖面上对应.可知本区横向上地温梯度变化较大.利用BSR资料估算了地温梯度并求得热流值.计算表明,地温梯度与热流值由西向东,随着离海沟距离的增大、离岛弧距离的减小而减小.BSR计算得到的热流值为28～64 mW/m2,与台湾西南实测热流值的结果基本可以对比. 相似文献
12.
分析了天然气水合物分解引起海底斜坡不稳定性的原因,探讨了水合物分解引起沉积物层孔隙压力变化规律.以南海北部神狐海域水合物样品钻获区为研究对象,应用极限平衡法探讨了海底无限斜坡的稳定性问题,计算了设定的不同滑动面的安全系数,建立了目标不稳定区相关参数条件下的水合物分解与海底斜坡不稳定的模式图,模拟计算了不同程度的水合物分解对海底斜坡失稳的影响作用.结果表明：在假设条件下,南海神狐海域当水深为1200 m,沉积物层厚度为200 m,对于20°的较大坡角,沉积物层中5%水合物分解将引起海底斜坡失稳;斜坡坡角为5°时,沉积物层中15%水合物分解后,将会引起海底斜坡失稳;当斜坡坡角为3°或更小时,沉积物层中25%水合物分解后,将会引起海底斜坡失稳. 相似文献
13.
本文采用AVO数值模拟方法,共选取水合物系统分层结构6个模型,对水合物、游离气和饱水沉积物接触界面的反射特征进行了数值模拟,研究了BSR及双BSR的存在条件与水合物体系垂向分布的关系,对一些现象从理论上进行了阐明.主要结论是：（1）强的似海底反射界面BSR与游离气体的存在密不可分,实际地震剖面中的“BSR”可能不对应水合物而只对应气体,无明显BSR的地方可能有水合物.（2）水合物顶部有可能存在游离气体,它可以在正常BSR（BSR1）之上形成另一个具有正极性的似海底反射界面BSR2.（3）正常BSR之下的双BSR（BSR0）其弹性机理有两种可能,一是水合物之下游离气上升迁移遇到某种阻隔层或不同气体组分的自然分层所造成的气体垂向分布的梯度性差异;二是当水合物之下的游离气体中存在残存的水合物时,同样会形成一定强度的似海底反射,在这种情形下BSR0的极性比较难以判断,取决于残存水合物上下游离气的饱和度和残存水合物的厚度. 相似文献
14.
南海北部陆坡具备天然气水合物成藏的基本地质条件,神狐海域天然气水合物是当前我国海洋天然气水合物勘探开发研究的重点靶区.然而,神狐海域水合物集中分布在水合物稳定带的底部薄层中,饱和度高,其水合物特征与典型的低甲烷通量控制的水合物分布有很大差异,对其成藏机理和控制因素尚不明确.本文构建了针对神狐水合物成藏过程的一维动力学模型,模型包括沉积压实作用、甲烷溶解度、以及水合物生成和沉积体渗透率,模拟计算的主控参量为海底沉积速率和水流通量,在孔隙水中甲烷浓度一定的情况下,水流速率决定了溶解甲烷的迁移速率和稳定带中甲烷的供给速率,并以此模型计算了神狐海域水合物聚集成藏的动力学过程.模型讨论了特定沉积速率和水流通量条件下水合物成藏与分布特征,并与实际观测数据进行比较研究.研究发现,基于当前沉积速率和水流通量条件模拟的水合物形成演化过程,与神狐海域实际水合物分布特征存在很大差异,但在假定系统中水合物饱和度初值达16~20%时,模拟的水合物饱和度分布特征与观测数据吻合,并因此推测在早期地质历史上,神狐海域存在更加丰富的甲烷水合物,当前的水合物分布特征是在对早期水合物继承基础上发展而成的,而且神狐海域水合物含量正逐渐减少. 相似文献
15.
南海琼东南盆地发现的高压泥底辟构造、海底“气烟囱”和天然气冷泉表明该地区可能存在着渗漏系统天然气水合物藏.假定在该区直径为1500 m的甲烷渗漏区内,甲烷渗漏通量为1000 kmol/a,甲烷水合物沉积层的温度范围为3~20 ℃,根据水合物条形移动界面理论建立传热模型,选取0 mbsf、100 mbsf、200 mbsf和425 mbsf分别计算在渗漏和扩散情况下的温度和生长速度变化曲线.结果表明甲烷水合物在沉积层骨架里的固结速度约为0.2 nm/s,经过约35000年后渗漏系统将演变成扩散系统.同时,甲烷水合物在渗漏系统里比在扩散系统里的生长速度快约20～40倍. 相似文献
16.
海底冷泉形成的一种可能机制是海平面下降引起天然气水合物的分解.本文基于对冷泉渗漏特征的分析,建立了二维轴对称模型,利用有限元方法定量分析了南海区域海平面下降对冷泉形成的影响.结果表明,末次冰盛期(26.5~19.0ka BP)海平面下降引起的冷泉活动可以持续到现在,但是从水合物停止分解至今,超孔隙压力的极值在持续减小,而流体向海底的渗漏达西速度先快速减小、然后缓慢减小.同时发现,流体向海底的渗漏达西速度与管状通道的渗透率、通道周围介质的渗透率以及通道的半径等有关,估计目前的冷泉活动还可以持续10000年以上.海平面下降引起的天然气水合物分解,可能是影响全球气候变化的一个重要因素. 相似文献
17.
已有的地质与地球物理信息表明南中国海北部陆坡神狐海域存在天然气水合物,2007年钻井和取样结果证实其以细颗粒均匀存在于水合物稳定带内,但区域分布范围极不规则.由于测井记录长度和取样深度的范围有限,天然气水合物垂向分布特征难以确定.为了深入了解此区域天然气水合物深度上的分布规律,对SH7井的多种测井数据进行综合分析并与地震反射特征建立联系,得到三个主要的沉积物性变化层位并以此为基础进行叠后数据的伪井约束反演,结果表明在已证实的含水合物层之下还存在高速层.而AVO叠前正演模拟分析结果与实际地震数据对比表明,研究区的天然气水合物稳定带可能由含水合物沉积物与饱水沉积物的薄互层组成,这就意味着在取样获得天然气水合物样品的深度之下,很可能存在另一个含水合物层. 相似文献
18.
J. Schneider von Deimling G. Rehder J. Greinert D.F. McGinnnis A. Boetius P. Linke 《Continental Shelf Research》2011,31(7-8):867-878
Tommeliten is a prominent methane seep area in the Central North Sea. Previous surveys revealed shallow gas-bearing sediments and methane gas ebullition into the water column. In this study, the in situ methane flux at Tommeliten is re-assessed and the potential methane transport to the atmosphere is discussed, with regards to the hydrographic setting and gas bubble modeling. We have compiled previous data, acquired new video and acoustic evidence of gas bubble release, and have measured the methane concentration, and its C-isotopic composition in the water column. Parametric subbottom sonar data reveal the three-dimensional extent of shallow gas and morphologic features relevant for gas migration. Five methane ebullition areas are identified and the main seepage area appears to be 21 times larger than previously estimated. Our video, hydroacoustic, subbottom, and chemical data suggest that ～1.5×106 mol CH4/yr (～26 tons CH4/yr) of methane gas is being released from the seepage area of Tommeliten. Methane concentration profiles in the vicinity of the gas seeps show values of up to 268 nM (～100 times background) close to the seafloor. A decrease in δ13C-CH4 values at 40 m water depth indicates an unknown additional biogenic methane source within the well oxygenated thermocline between 30 and 40 m water depth. Numerical modeling of the methane bubbles due to their migration and dissolution was performed to estimate the bubble-derived vertical methane transport, the fate of this methane in the water column, and finally the flux to the atmosphere. Modeling indicates that less than ～4% of the gas initially released at the seafloor is transported via bubbles into the mixed layer and, ultimately, to the atmosphere. However, because of the strong seasonality of mixing in the North Sea, this flux is expected to increase as mixing increases, and almost all of the methane released at the seafloor could be transferred into the atmosphere in the stormy fall and winter time. 相似文献
19.
本文研究了多组分天然气在海底沉积层中稳定区和存在区的一些特点. 首先,考虑盐的浓度的影响,建立了天然气含有甲烷和丙烷两种组分的水合物形成的相变曲线,即温度和压力关系曲线,同时也建立了甲烷和丙烷两种组分天然气溶解度的加权关系. 运用水合物预测模型,计算了多组分天然气水合物在海底沉积层中的稳定区及存在区,并同单组分的甲烷水合物的结果进行了对比.计算表明：两种组分的天然气水合物的稳定区与单组分甲烷水合物的稳定区有较大差别,这归因于丙烷对相变曲线大的影响;当天然气浓度大于对应的溶解度时,水合物将形成,由此决定了存在区域;稳定区和存在区范围都受到丙烷含量的较大影响,盐度的增大则减少了稳定区范围. 最后对甲烷分别与其他气体（例如二氧化碳,乙烷和硫化氢等）组合的天然气水合物形成的稳定区范围进行了简要的分析. 相似文献
20.
Ji-Hoon Kim Myong-Ho Park Urumu Tsunogai Tae-Jin Cheong Byong-Jae Ryu Young-Joo Lee Hyun-Chul Han Jae-Ho Oh Ho-Wan Chang 《Island Arc》2007,16(1):93-104
Abstract Geochemical analyses of sediments, pore water and headspace gas of the piston cores taken from the eastern part of Ulleung Basin of the East Sea (Japan Sea) were carried out to assess the origin of the sedimentary organic matter and interstitial fluid. Several tephra layers within the core are identified as the Ulleung‐Oki (10.1 ka), the Aira‐Tanzawa (23 ka) and the Ulleung‐Yamato (30.9 ka) tephras. With the exception of these volcanic layers, the cores consist predominantly of muddy sediments that contain >0.5% total organic carbon. Atomic C/N ratios and δ13Corg values suggest that the organic matter originated from marine algae rather than from land vascular plants, whereas Rock‐Eval pyrolysis suggests that the organic matter is thermally immature and comes from a land vascular plant (Type III). These conflicting results seem to be caused by the heavy oxidization of the marine organic matter. Sulphate concentration profiles of pore waters show strongly linear depletion (r2 > 0.97) with sediment depth. The estimated sulphate–methane interface (SMI) depth using the sulphate concentration gradient was nearly 3.5 m below seafloor (mbsf) in the southern part of the study area, and deeper than 6 mbsf in the northern part of the area. The difference in SMI depths is likely associated with the amount of the methane flux. The methane concentration below the SMI in the two southern cores increases rapidly, implying the occurrence of methanogenesis and anaerobic methane oxidation (AMO). In contrast, the two northern cores have a low methane concentration below the SMI. values measured from all cores were in the range of −83.5 to −69.5‰, which suggests that the methane derives from a methanogenic microbe. values become decreased toward SMI, but increased below SMI; therefore, has eventually the minimum value near the SMI. The values are also decreased when the methane concentration is increased. These phenomena support the typical occurrence of AMO in the study area. 相似文献