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近23年的调查研究，使我们认识到分布于洋中脊、弧后盆地、岛弧和热点等环境的海底热液活动发育在多种围岩类型之上，包括超基性岩石、基性岩石、中性岩石、酸性岩石和沉积物。海底热液活动经历了岩浆去气作用、流体-岩石/沉积物相互作用和流体-海水混合，获取了岩浆、岩石、海水和沉积物的物质，构成了热液循环，产生了高温、低氧、高或低pH值、富含Fe、Mn、Cu、Zn、Pb、Hg、As等元素以及气体组分（甲烷、氢等）的喷口流体，影响了海水、沉积、岩石和生物环境，形成了热液柱、硫化物、含金属沉积物和蚀变岩石等热液产物，组成了海底热液系统。未来，促进海底热液活动探测技术和热液产物测试方法的发展，对海底热液区的岩石、喷口流体、热液柱、硫化物、含金属沉积物以及热液循环、生物活动的持续观测与研究，无疑将为人类探知海底地质过程及生命活动、保护海底热液环境和合理开发利用海底资源提供有力的工作支撑。 相似文献
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本文以冲绳海槽伊平屋北部热液区(126o53.80′,27o45.50′)的现场水文数据作为背景条件,使用k-ε湍流模型模拟热液柱的动力过程。模拟计算得到的羽流速度、温度和湍流耗散率等基本物理量展现了热液柱的时空演化过程。模拟结果显示,羽流最大上升高度及中性浮力面高度与海底的距离分别为83.62m和68.97m,和2014年先导专项在此附近热液区所观测的温度异常和盐度异常的深度位置(离海底约66—86m)接近。羽流的上升速度满足高斯分布,其半径b与距喷口高度z-H成正比:b=0.0985(z-H),其中z为距海底高度,H为热液烟囱体的高度。羽流的最大体积通量比喷口的初始值增加了878倍,达1.034m~3/s;在中性浮力面位置附近,动量通量达到最大值,为0.156m~4/s~2,比初始值增加了882倍;浮力通量在中性浮力面以下和BM2000(Bloomfield et al,2000)理论模型符合良好,在中性浮力面以上则呈现随高度先增加后减小的特征。本文计算得到的平均卷挟率为α≈0.0807,与背景流较弱的热液区的声学现场观测结果相符。 相似文献
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洋中脊的水下热液喷口喷出热的缺氧流体,当它们从海底喷出时与周围海水激烈混合,沉淀出各种硫化物和氧化物,直到达到海底之上数百米平衡为止。最终的热液柱沿等密度面散布,等密度面处的热液柱可由溶解的化学示踪物高度富集和悬浮颗粒负载增高检验出来。最近的研究中,... 相似文献
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深海热液流体与周围海水之间存在明显的物理和化学差异,通过检测海水的位温浊度异常是探测深海热液活动的重要手段之一。本文采用"海底火山带项目（Submarine Ring of Fire 2002）"拖曳式温盐深测量仪数据资料,研究了东北太平洋Explorer Ridge热液场的水文特征及物质能量通量的释放。结果表明Explorer Ridge热液场热液羽状流中性浮力层所在深度范围约为1 600~1 900 m,距离海底的高度约为200 m,最大位温、盐度和浊度异常分别为0.04℃、0.004和0.18 NTU;中性浮力层热液羽状流帽呈椭圆结构,其长轴与洋中脊线重合,羽状流帽总面积约为27 km2;热液羽状流在中性层范围内存在明显的分层现象,通过经验公式计算得到Explorer Ridge热液场观测范围内热液喷口的总的浮力通量为6.19×10-2 m4/s3,平均值为2.063×10-2 m4/s3;总的体积通量为9.884×10-2 m3/s,平均值为3.295×10-2 m3/s;总的热通量为194.9 MW,平均值为64.967 MW。 相似文献
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海底热液活动调查研究是深海进入、深海探测和深海开发的切入点之一。近十年来,中国在西太平洋弧后盆地、东太平洋海隆、大西洋洋中脊和印度洋脊,发现了一批新的海底热液活动区,围绕着热液活动区的硫化物、流体、热液柱、生物等热液产物开展了调查研究,构建了海底热液地质学,提出了热液活动、冷泉及天然气水合物的同源异汇假说,出版了《海底热液地质学》、《现代海底热液硫化物成矿地质学》、《现代海底热液活动》、《东太平洋海隆热液地质》专著,获得了一批调查研究成果。未来,聚焦海底热液活动的深部过程及其资源环境效应关键问题,发展海底热液活动探测技术,拓展极地海底热液活动调查研究新领域,围绕烟囱体、热液柱、含金属沉积物、流体以及热液区生物等热液产物,开展深入、系统的调查研究工作,无疑将推动海底热液地质学取得新的进展。 相似文献
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快速扩张的东太平洋海隆侧翼年轻深海丘陵的热液释放现象 总被引：2，自引：0，他引：2
大洋板块从洋中脊扩张后,经过热传导和热平流,大洋岩石圈冷却下来。据估算,50%的水热损失(5.5×1012W)和流体通量(2.3×1012m3/a)来自于5Ma或者更年轻的海底。来自0.1～5Ma的地壳流体循环的大量矿物沉降,可以解释地震速度的快速增加,上地壳孔隙度和渗透率随年龄增加而降低,以及504B孔岩心中约6.9Ma时的玄武岩蚀变和矿脉层。虽然发现了洋脊侧翼通量增大的证据,但是由于缺少勘探和足够的知识来了解洋脊侧翼的热液如何释放至海底,对于如此大范围的海底热液喷口的直接观察进行地很少。沿着洋中脊顶部已经发现了上百座活动喷口,在这里已经进行… 相似文献
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硬石膏是最早构成热液烟囱体壁的矿物之一,其对于了解流体-海水混合以及海底热液系统中元素的迁移与循环具有重要的意义。为此,对西太平洋冲绳海槽唐印热液区中的硬石膏,进行了微区原位元素以及硫同位素组成分析。根据硬石膏的结晶形态,可以将硬石膏分为两种类型：较早形成的I型硬石膏,其呈半自形或他形晶,似针状、放射状及不规则晶的集合体产出;较晚形成的II型硬石膏,其呈自形晶,以板状及粒状晶的集合体产出。当热液流体初次遇到海水时,将快速沉淀形成I型硬石膏,并构成了热液烟囱体的壁。随后,II型硬石膏经历了一个相对充分的生长阶段。同时,硬石膏中的Ba、Al、Sr、Ni、Fe、Mn和Cr含量明显高于海水,表明产生硬石膏沉淀的热液流体来自于海底面以下,是经历了流体-岩石和/或沉积物相互作用的流体。硬石膏的Mg含量明显分别低于海水和高于喷口流体,表明其是流体-海水混合的结果。I型硬石膏,其Sr含量明显低于II型硬石膏,表明在形成自形、板片状或粒状硬石膏的期间,来自热液流体的Sr,主要进入II型硬石膏中。硬石膏的Fe、As、Sr、Ba和Pb含量,明显高于冲绳海槽喷口流体的,则表明这些来自流体中的元素更容易随着硬石... 相似文献
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冲绳海槽中部Jade热液活动区中海底热液沉积物的硫同位素组成及其地质意义 总被引：12，自引：3，他引：9
测定了冲绳海槽中部Jade热液活动区中18个热液沉积物样品的硫同位素组式,其中10个硫化物样品的δ34S值为5.2×10-3～7.2×10-3,7个硫酸盐样品的34S值为16.3×10-3～22.3×10-3,1个自然硫样品的δ34S值为8.2×10-3热液沉积物的硫主要来自中、酸性火山岩和海水,并且在流体与沉积物相互作用过程中海底沉积物也可能为热液沉积物的形成提供部分的硫.导致本区热液沉积物中硫化物与其他热液活动区的硫同位素组成不同的原因,主要是各热液活动区的硫源以及有关岩浆活动和构造演变的不同.海底热液体系中硫的演化是一个复杂的过程,涉及被加热海水的上升、流体与火山岩的相互作用、海水硫酸盐和中、酸性火山岩中流的混合作用以及流体与沉积物相互作周等一系列海底热液活动,其中海水和中、酸性火山岩的相互作用是本区硫演化的一个重要机制. 相似文献
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大型海底热液硫化物矿体的形成机制是涉及多种控制因素的复杂地质过程,其中热液流体同海水的混合扮演着重要角色。大洋钻探计划(ODP)资料表明在大西洋TAG区热液硫化物矿体内部,热液流体同经过改造的海水之间发生着广泛的混合作用,这个过程在很大程度上控制着海底热液硫化物矿体的内部结构和化学组成。以TAG热液硫化物矿体为例,利用数值模拟方法模拟了热液流体与经过不同程度改造的海水的混合过程,试图探讨海水与热液流体混合在热液硫化物矿体形成中的作用。模拟计算结果表明:(1)来自矿体深部的热液流体与经围岩加热的下渗海水的混合是造成TAG热液活动区硬石膏大量沉淀的重要原因;(2)在热液流体与海水的混合过程中,混合流体的化学性质和矿物沉淀情况在330~310℃上下发生了较大变化,330~310℃是一个特殊的温度区域;(3)利用数值计算结果探讨了TAG热液活动区不同区块(TAG-1,TAG-2和TAG-5等)的流体混合作用和热液活动过程。 相似文献
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热液羽状流是海底热液活动的重要标志，海底多金属硫化物是热液活动的产物。现阶段洋中脊多金属硫化物勘探工作的第一步是开展热液羽状流的近底探测；综合各类异常信息，实现从发现热液活动喷口到发现矿床的突破。本文以热液羽状流为研究对象，从羽状流的近底探测、扩散机制和分布特征3个方面，概述了最新的研究进展和有待完善的方面，阐述了羽状流在洋中脊多金属硫化物找矿中的指示作用，最后总结性地指出时空连续性、参数多元化将是热液探测的发展趋势，有助于提升对热液羽状流分布特征的认识，将为热液区分布模式的研究提供更加精细的探测资料。 相似文献
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A computational fluid dynamics (CFD) model was developed to simulate the turbulent flow and species transport of deep-sea high temperature hydrothermal plumes. The model solves numerically the density weighted unsteady Reynolds-averaged Navier–Stokes equations and energy equation and the species transport equation. Turbulent entrainment and mixing is modeled by a k–ε turbulence closure model. The CFD model explicitly considers realistic vent chimney geometry, vent exit fluid temperature and velocity, and background stratification. The model uses field measurements as model inputs and has been validated by field data. These measurements and data, including vent temperature and plume physical structure, were made in the ABE hydrothermal field of the Eastern Lau Spreading Center. A parametric sensitivity study based on this CFD model was conducted to determine the relative importance of vent exit velocity, background stratification, and chimney height on the mixing of vent fluid and seawater. The CFD model was also used to derive several important scalings that are relevant to understanding plume impact on the ocean. These scalings include maximum plume rise height, neutrally buoyant plume height, maximum plume induced turbulent diffusivity, and total plume vertically transported water mass flux. These scaling relationships can be used for constructing simplified 1-dimensional models of geochemistry and microbial activity in hydrothermal plumes. Simulation results show that the classical entrainment assumptions, typically invoked to describe hydrothermal plume transport, only apply up to the vertical level of ~0.6 times the maximum plume rise height. Below that level, the entrainment coefficient remains relatively constant (~0.15). Above that level, the plume flow consists of a pronounced lateral spreading flow, two branches of inward flow immediately above and below the lateral spreading, and recirculation flanking the plume cap region. Both turbulent kinetic energy and turbulence dissipation rate reach their maximum near the vent; however, turbulent viscosity attains its maximum near the plume top, indicating strong turbulent mixing in that region. The parametric study shows that near vent physical conditions, including chimney height and fluid exit velocity, influence plume mixing from the vent orifice to a distance of ~10 times the vent orifice diameter. Thus, physical parameters place a strong kinetic constraint on the chemical reactions occurring in the initial particle-forming zone of hydrothermal plumes. 相似文献
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Basic mathematical model for the normal black smoker system and the hydrothermal megaplume formation
A tube model to simulate the normal black smoker system has been built, where the Darcy flow equation, the Ergun equation and the turbulent pipe flow equation are used respectively to describe the dynamic process of different key areas in the hydrothermal circulation system. At the same time, a convection-diffuse Equation for the temperature field is used for describe the exchange of thermal energy and the law of temperature variation. Combining the above facts and using efficient mathematical algorithms and programming with the MatLab programming language, the variation curves of temperature, pressure and mass flow rate are determined, while also the dynamic heat equilibrium and pressure equilibrium within the black smoker system are analyzed. On the basis of the model of the normal black smoker system, a megaplume formation model is further built. For instance, the hydrothermal venting plume on the Juan de Fuca Ridge has been simulated and the simulation results are fairly consistent with Baker's imputed data in 1986. On the basis of the above productive simulation, a series of factors for megaplume formation and the effectiveness of the main parameters of the periodicity of the megaplume formation, temperature and the maximum mass flow rate are systematically discussed. Main conclusions are as follows: The normal black smoker system can evolve into a megaplum eruption. In fact, the passageway of the hydrothermal discharge is blocked by the hydrothermal sediments during the black smoker period, which leads to a hydrothermal fluid accumulation, rise of temperature and increase of buoyancy pressure under the seabed. After a period of 2~3 a, the megaplume hydrothermal eruption will occur when the increasing buoyancy pressure is high enough to crack the blockage (cap).Meanwhile, the temperature of the heat source must exceed 500 ℃, while the highest temperature of the eruption fluid may be high up to 413 ℃, which is fairly consistent with the surveying data.If the temperature of the heat source were to be higher than 500 ℃, then the critical period for the megaplume formation could be obviously curtailed to be less than 1 a, while the critical temperature and the maximum mass flow rate are nearly invariable. As the permeability increases, the maximum mass flow rate increases gradually close to a steady value. 相似文献
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建立了一种新的管状模型来模拟普通黑烟囱体的热液循环系统,分别用达西方程、湍流方程、Ergun方程和“浮压力差”方程来描述热液循环不同关键环节处的动力学系统,用一个温度场的对流-扩散方程来描述反应区的热能交换及系统的温度变化规律.在联立几个方程并用有效的数值算法及Matlab语言编程求解后,得出了系统中温度、压力及物质流速随时间的变化曲线,并对黑烟囱体内部的动态热平衡和压力平衡进行了分析.在普通黑烟囱体系统模型的基础上进一步建立了巨型羽状流(巨羽流)生成的数学模型.选择胡安·德富卡(Juan de Fuca)洋脊热液喷口对巨羽流的形成进行了模拟,其结果与Baker根据实测数据估算的近似值吻合很好.在上述模型的基础上进一步探讨了巨羽状流形成的一系列条件及主要参数对巨羽流生成周期、温度和最大物质流速等的影响.主要结论如下:巨羽流系统可以由普通黑烟囱系统发展演化而成,其实际过程是普通黑烟囱流系统活动所形成的热液沉积在一定程度上会堵塞热液喷溢通道(相当于形成盖层),造成热液在海底之下积蓄和升温,从而导致浮压力差增大,经过2~3 a(浮压力差达到盖层破裂极限值)则可形成巨羽流系统,巨羽流产生时的热源温度必须超过500℃,喷出热液的最高温度为413℃左右(与实际观测到的海底热液的最高温度一致).当反应区热源温度增大时,产生巨羽流的临界时间明显变短(可能不到1 a),而临界温度(巨羽流生成时的温度)及巨羽流的最大物质流速几乎不随其变化;随着渗透率的增大,巨羽流的最大物质流速也随之增大,但其增速随渗透率的进一步增大而变缓,并逐渐趋向一个相当于下渗流无摩擦阻力时的极限稳定值. 相似文献
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李粹中 《海洋地质与第四纪地质》1992,12(4):75-86
海底扩张中心的热液矿化作用是国际地球科学研究中最为活跃的领域之一。本文介绍了:1.热液多金属矿床调查的历史沿革;2.九十年代热液多金属矿床的海上调查方法;3.海底热液矿床的赋存条件;4.海底热液矿化作用过程;5.高强度热液活动与地质构造事件;6.热液矿体形状和流体动力学。作者认为,在我国开展太平洋多金属结核资源调查的同时,应对热液矿床的研究给予足够的重视。 相似文献
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Metal-enriched minerals have been widely observed near hydrothermal vent fields.However,the dynamics of particulate metals influenced by hydrothermal activities is poorly constrained.Here,radioactive ~(234)Th in both dissolved and particulate phases were used to examine the kinetics of particle-reactive metal adsorption,removal,and residence in a newly found hydrothermal plume over the Southwest Indian Ridge.The results showed a relatively low value on ~(234)Th/~(238)U ratios(i.e.,0.73-0.88) compared to the deep oceans,indicating an enhanced adsorption of particle-reactive metals onto particulate matter in the plume.Based on the ~(234)Th-~(238)U disequilibria,the adsorption and sinking rate constants of ~(234)Th averaged(0.009±0.001) d~(-1) and(0.113±0.024) d~(-1) in the hydrothermal plume,corresponding to the residence times of(115±19) d and(16±5) d for dissolved and particulate ~(234)Th,respectively.This timescale allows vent-discharged particle-reactive metals to disperse hundreds to thousands of miles away.Thus,hydrothermal activities might influence the metal distribution in deep ocean over a very large scope.Also,a high sinking flux of(36.2±5.4) B q/(m~2·d) for ~(234)Th was observed for the plume,suggesting an enrichment of metal in particles deposited close to the vent.The enhancement of particle sinking could also benefit the transport of organic carbon and nitrogen and fuel the benthic ecosystems under the plume regimes.Thus,hydrothermal plumes may have an impact on both the elemental geochemistry and/or ecosystem to the deep oceans interior than previous expectation. 相似文献
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Spatial distribution pattern of seafloor hydrothermal vents to the southeastern Kueishan Tao offshore Taiwan Island 总被引：1，自引：0，他引：1
HAN Chenhu YE Ying PAN Yiwen QIN Huawei WU Guanghai CHEN Chen-Tung Arthur 《海洋学报(英文版)》2014,33(4):37-44
Investigations of the diffusion activities both within and outside the seafloor hydrothermal vents, as well as related mineral genesis, have been one of the key focuses of ocean biogeochemistry studies. Many hydrothermal vents are distributed close to the southern Okinawa Trough on the less-than-30-m deep shallow seafloor off Kueishan Tao, northeast of Taiwan Island. Investigations of temperature, pH and Eh at four depths of hydrothermal plume were carried out near Kueishan Tao at the white(24.83°N, 121.96°E) and yellow(24.83°N, 121.96°E) vents. An 87 h of temperature time series observation-undertaken near the white vent showed that tide is the main factor affecting the background environment. Based on the observed data, 3-dimensional sliced diffusion fields were obtained and analyzed. It was concluded that the plume diffused mainly from north to south due to ebb tide. The yellow vent's plume could effect as far as the white vent surface. From the temperature diffusion field, the vortices of the plume were observed. The Eh negative abnormality was a better indicator to search for hydrothermal plumes and locate hydrothermal vents than high temperature and low pH abnormalities. 相似文献