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1.
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
2.
在简单巨羽流生成模型基础上,考虑下渗海水对循环热液的稀释作用设计建立了管状模型,旨在讨论下渗海水(在海底普遍存在)对热液循环系统的影响。在保持原模型基本结构的基础上又添加了代表下渗低温海水稀释作用的D区。模型着重对D区中的低温下渗海水(未经反应区加热)与释放区热液的混合,从而对实现热液稀释的作用进行分析。首先建立系统中两个循环体的控制方程,然后在有限条件下对模型求解,并对求解的结果进行实际意义的分析。主要结论包括下渗区D区作为释放区时,D区释放流体的物质流速已明显大于C区中流体的物质流速,下渗区成为另一个喷溢区;如果在烟囱体下部有裂缝或者其外壳的渗透率较高时,对系统所释放流体的温度、物质通量等指标的估算不能再按常规方法单纯地考虑烟囱体的喷口,因为周围的"高渗区"可能是更大的释放区;对于巨羽流系统,由于释放区C区的压力较小,所以不太可能发生上述情况;具有明显低温流的天然系统不可能位于本模型的参数空间;对热液系统发育的不同阶段应采用不同的数学模型。 相似文献
3.
为了重建EPR 9°~10°N L喷口的形成环境,采用矿物学、地球化学及年代学的方法,对黑烟囱体的矿物组成、矿物结构、元素剖面分布以及黑烟囱体内外层铅-210测年进行了研究。矿物学观察表明,该喷口烟囱体内壁主要由方黄铜矿组成,而外壁则主要由硬石膏组成。铅-210测年结果表明,烟囱体形成于EPR 9°~10°N区域内1991年的火山喷发事件之后,并有较低的生长速率,约为0.3cm/a。结合该喷口及其附近A喷口已发表资料认为,该烟囱体开始生长是由于蒸气相流体引起的,其后期受到卤水相流体的影响,而且流体温度应不小于330℃。 相似文献
4.
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
5.
热液流体在物理化学特征方面与周围海水存在较大差异,探测温度异常和浊度异常是寻找热液羽状流信号的重要手段。本文采用“大洋一号”科考船第20航次的拖曳CTD数据和浊度数据,以及21航次的定点CTD数据,研究了西南印度洋龙方斤热液区的温度异常和浊度异常现象。研究表明热液区中性浮力层在水深2 550~2 650 m间,厚度约为100 m,温度异常达0.01 ℃;水深 2 750~2 800 m间亦有温度异常,最大可达0.08 ℃;温度异常水深处存在相应的浊度异常。深层背景海水位温和位密间存在简单线性关系。此外,经初步估计,热液活动区初始浮力通量为8.78×10-4 m4/s3;通过中性浮力层估算热液热通量,约为130±43 MW。 相似文献
6.
现代海底热液活动的热和物质通量估算 总被引：4，自引：3，他引：4
对现代海底热液活动所导致的热和物质的通量研究是非常重要的,因为这不仅涉及到海洋环境研究的基础,而且涉及到海水性质的历史演化.当前对热通量估算的主要依据是来自对热液烟囱、低温扩散流及洋中脊的观测数据, 然而在对烟囱体热通量的估算中很少考虑同时存在的传导项,半空间冷却模型的热通量密度函数与实际数据误差较大.因此,应用了三种方法重新估算了热液活动的热通量:(1)通过烟囱体及扩散流估算的热液热通量为97.359 GW;(2)通过热液羽状体估算的热通量为84.895 GW;(3)利用所提出的指数衰减法,通过洋壳传导通量估算的热通量为4.11 TW.对物质通量估算的研究较少,其原因是现场观测数据太少.以大西洋中脊TAG区热液流体为代表首次估算了不同元素的物质通量.用不同方法所得估算值的差异反映了人类对热液活动的认知程度,系统地现场观测将有助于准确估算热液活动对海洋的贡献. 相似文献
7.
ZHAI Shikui WANG Xingtao YU Zenghui 《海洋学报(英文版)》2006,25(6):43-51
Research on heat and mass flux yielded by modern seafloor hydrothermal activity is very important, because it is involved not only in the base of ocean environment research, but also in the historical evolution of seawater properties. Currently, estimating heat flux is based on the observation data of hydrothermal smokers, low-temperature diffusive flow and mid-ocean ridge mainly. But there are some faults, for example, there is lack of a concurrent conductive item in estimating the heat flux by smokers and the error between the half-space cooling model and the observation data is too large. So, three kinds of methods are applied to re-estimating the heat flux of hydrothermal activity resepectively, corresponding estimation is 97. 359 GW by hydrothermal smoker and diffusive flow, 84.895 GW by hydrothermal plume, and 4. 11 TW by exponential attenuation method put forward by this paper. Research on mass flux estimation is relatively rare, the main reason for this is insufficient field observation data. Mass fluxes of different elements are calculated using hydrothermal vent fluid data from the TAG hydrothermal area on the Mid-Atlantic Ridge for the first time. Difference of estimations by different methods reflects the researching extent of hydrothermal activity, and systematically in - situ observation will help to estimate the contribution of hydrothermal activity to ocean chemical environment, ocean circulation and global climate precisely. 相似文献
8.
1Introduction Heat flux yielded by modern seafloor hydrother-mal activity could be next only to heat radiation fromthe sun to the earth, and be similar to energy pro-duced by volcanism. And mass flux of hydrothermalactivity could be close to that of river… 相似文献
9.
10.
The approach to determine working frequencies of acoustic in-situ detector for seafloor hydrothermal fluid is presented. Based on the research of deep-sea noise and the sound generated by mid-ocean ridge black smoker hydrothermal vents, and on the hydrothermal-vent animal hearing ranges, coupled with influences of suspended particles of hydrothermal on acoustic attenuation under different frequencies, the optimal frequency range for detection of acoustical signal near black smokers is determined. The optimal frequencies providing the maximum ratio of receiver signal to background noise are obtained. We have developed a laboratory experimental setup for the optimal frequencies selection. In particular, we evaluated time-of-flight performance with respect to the source signal parameters of center frequency and bandwidth. The experimental results confirm the effectiveness of our approach. Current results indicate that individual transducers operated in the range of 18 ～ 25 kHz are immune to most interfering sounds and suitable for our system. 相似文献
11.
We develop and apply visualization and quantification methods to reconstruct hydrothermal plumes in 3D from acoustic images and to make the first direct measurements from the reconstructions of scalar properties that describe the behavior of two buoyant plumes discharging from adjacent black smoker chimneys. The actual behavior is then compared to that predicted by a classic simple buoyant plume model. The images are reconstructed as isointensity surfaces of backscatter from particulate matter suspended in the plumes. The measurements pertinent to the role of the plumes as agents of dispersal of heat and mass into the ocean include change with height of diameter, particle distribution, dilution, centerline attitude, surface protrusions, and connectivity. The protrusions are the surface expression of eddies and appear to follow a bifurcating helical flow pattern that resemble simulation of the naturally forced flow of coherent vortex rings as the eddies rise with the buoyant plume. These direct measurements and the derived entrainment coefficient are generally consistent with behavior predicted by the simple buoyant plume model and support engulfment by vortex shedding as a primary mechanism for entrainment of surrounding seawater. Deviations from predicted buoyant plume behavior are diagnostic of particle dynamics. 相似文献
12.
J. Sarrazin P. Rodier M.K. Tivey H. Singh A. Schultz P.M. Sarradin 《Deep Sea Research Part I: Oceanographic Research Papers》2009,56(11):2065-2074
Numerous attempts have been made over the last thirty years to estimate fluid flow rates at hydrothermal vents, either at the exit of black smoker chimneys or within diffuse flow areas. In this study, we combine two methods to accurately estimate fluid flow velocities at diffuse flow areas. While the first method uses a hot film anemometer that performs high-frequency measurements, the second allows a relatively rapid assessment of fluid flow velocity through video imagery and provides in situ data to calibrate the sensor. Measurements of flow velocities on hydrothermal diffuse flow areas were obtained on the Mid-Atlantic Ridge (MAR). They range from 1.1 to 4.9 mm/s at the substratum level, in low-temperature (4.5–16.4 °C) diffuse flow areas from the Tour Eiffel sulfide edifice. A strong correlation was observed between fluid flow velocities and temperature, supporting the possible use of temperature as a proxy to estimate the flow rates in diffuse flow areas where such a simple linear flow/temperature relation is shown to dominate. 相似文献
13.
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
14.
选取胡安.德富卡洋脊(Juan de Fuca Ridge,JDFR)因代沃(Endeavour)段的17个热液黑烟囱体样品对其中的硫同位素进行分析测定,讨论了因代沃段热液活动区内黑烟囱体成矿的物质来源、将硫同位素数据与已发表的热液流体及硫化物数据耦合,并结合前人的成果得到如下认识:(1)因代沃段硫化物的硫同位素组成与其他无沉积物覆盖的洋脊硫化物硫同位素组成相似,然而其相比于南胡安.德富卡洋脊(South Juan de Fuca Ridge,SJFR)硫化物亏损重同位素;(2)结合前人研究成果,如果SJFR硫化物的硫全部来自基底玄武岩的淋洗与海水中的硫酸盐,那么因代沃段硫化物的硫可能有1%～3%来自沉积物的贡献,故提出因代沃段成矿系统中的硫来源主要来自基底玄武岩,同时伴随有少量海水硫酸盐来源及沉积物来源的硫加入;(3)将硫同位素数据与已发表的热液流体及硫化物数据进行耦合发现热液流体中的沉积物信号与硫化物中的硫可能来自不同的源,并提出沉积物端元可能位于下渗区。 相似文献
15.
选取胡安·德富卡洋脊(Juan de Fuca Ridge,JDFR)因代沃(Endeavour)段的17个热液黑烟囱体样品对其中的硫同位素进行分析测定,讨论了因代沃段热液活动区内黑烟囱体成矿的物质来源、将硫同位素数据与已发表的热液流体及硫化物数据耦合,并结合前人的成果得到如下认识:(1)因代沃段硫化物的硫同位素组成与其他无沉积物覆盖的洋脊硫化物硫同位素组成相似,然而其相比于南胡安·德富卡洋脊(South Juan de Fuca Ridge,SJFR)硫化物亏损重同位素;(2)结合前人研究成果,如果SJFR硫化物的硫全部来自基底玄武岩的淋洗与海水中的硫酸盐,那么因代沃段硫化物的硫可能有1%~3%来自沉积物的贡献,故提出因代沃段成矿系统中的硫来源主要来自基底玄武岩,同时伴随有少量海水硫酸盐来源及沉积物来源的硫加入;(3)将硫同位素数据与已发表的热液流体及硫化物数据进行耦合发现热液流体中的沉积物信号与硫化物中的硫可能来自不同的源,并提出沉积物端元可能位于下渗区。 相似文献
16.
深海在黑暗、高静水压、低温（黑烟囱等热液系统除外）和寡营养的极端环境下形成了特殊的生境。对深海生物/微生物的研究,不仅可以揭示各种深海生物的生理代谢特性和动态变化规律,而且有助于深海生物资源的开发利用,特别是深海微生物碳循环机制的相关研究可为全球实现碳中和目标提供新的路线图。研究深海生物的首要条件是获得大量保持原位特性的样本,然而传统深海采样手段的局限可能导致深海相关研究结果无法反映深海环境下真实的生命过程,亟需发展满足深海生物原位研究的采样方法和生态监测技术。本文对深海生物研究现状,相关科学问题和原位组学研究进展,以及原位生态监测装备研发和应用进行综述,并对深海原位生物实验室进行了展望。 相似文献
17.
热液系统输向大洋的热通量估算 总被引：5，自引：1，他引：5
从四个方面对现代海底热液活动输向大洋的热通量进行了初步估算.热液系统通过集中、高温的热液烟囱和低温、大面积漫溢热水的形式向海洋输送的热通量为357GW;由底热异常边界层计算出的热通量为32GW;根据Baker提出的扩张洋脊的扩张速率和扩张洋脊热液柱覆盖率之间的线性关系,推算的热液通量为1086GW;根据扩张洋脊岩墙冷却和扩张推算的热通量为592GW.不同的方法给出的结果有较大的差异.一方面这些结果反映了热液系统向大洋的供热水平,另一方面反映了目前对现代海底热液活动的认识水平.虽然热液系统向大洋的热输出比太阳的热辐射小,但由于其特殊的供热方式,这部分热能仍有可能对全球气候带来影响,应在今后的研究中给予重视. 相似文献
18.
Geologic setting of the Snake Pit hydrothermal site: An active vent field on the Mid-Atlantic Ridge 总被引：2，自引：0，他引：2
TheSnake Pit Hydrothermal Site lies on the axis of the Mid-Atlantic Ridge at 23°22′ N latitude, about 30 km south of the Kane Transform
Intersection. Active ‘black smoker’ vents and a surrounding field of hydrothermal sediment occur at the crest of a laterally
extensive neovolcanic ridge. It is one of the first active hydrothermal vent fields to be found on a slow-spreading ridge
axis and despite significant differences in its geologic setting from those of the East Pacific Rise, has many similarities
to its fast-spreading counterparts. Although preliminary reports have documented many interesting aspects of these vents and
their surroundings, new data collected from the manned submersible ALVIN and the deep-towed ANGUS camera system define the
regional tectonic setting as well as the local geologic environment of this fascinating area.
The Snake Pit vents are located on a local peak of a volcanic constructional ridge at a depth of 3450 m, 700–800 m deeper
than vents known from the East Pacific Rise, Galapagos, or Juan de Fuca spreading centers. The vent field is at least 600
m long and up to 200 m wide and is covered by a thick blanket of greenish to yellow-orange hydrothermal sediment. Both active
and extinct vents are perched along the crests of steep-sided sulfide mounds that reach heights of over 40 m. High-temperature
(350° C) fluids are vented from black smoker chimneys and low-temperature (226° C) fluids seep from sulphide domes and subordinate
anhydrite constructions. Water temperatures, flow rates, fluid chemistries, and mineralization are strikingly similar to vents
of faster spreading ridge crests; however, a somewhat distinct fauna inhabit the area. 相似文献
19.
Considerable effort has been expended in studying the Izu-Bonin Arc over the past 15 years. In particular, 43 dives of the Shinkai 2000 have been undertaken there to discover and evaluate the extent of submarine hydrothermal activity and mineraliza tion. Most effort has been focused on Myojin Knoll (23 dives), Suiyo Seamount (6 dives), and Kaikata Caldera (10 dives). The Izu-Bonin Arc is divided in two by the Sofugan Tectonic Line. Eight submarine caldera are located north of this line but only one is south of it. The physiography of the northern sector of the arc is quite different from that of the southern sector. Volcanic rocks from the northern sector are more acidic than those from the southern sector. Evidence for submarine hydrothermal mineralization has been observed at four seamounts along the Izu-Bonin Arc (Myojin Knoll, Myojinsho, Suiyo Seamount, and Kaikata Caldera), and submarine hydrothermal activity is evident at another three seamounts along the arc (Kurose Hole, Mokuyo Seamount, and Doyo Seamount). The most extensive submarine hydrothermal mineral deposit so far located on the Izu-Bonin Arc is the Sunrise deposit at Myojin Knoll. This deposit, at least 400 m in diameter and 30 m high, is associated with black smoker venting, inactive sulfide chimneys, massive sulfides, hydrothermal Mn crusts, and a hydrothermal vent fauna. The maximum recorded temperature of the hydrothermal vents there was 278°C. Some of the sulfide chimneys contained as much as 49 μg / g Au and 3,400 μg / g Ag. The sunrise deposit is one of the largest submarine volcanic massive sulfide deposits so far discovered in midocean ridge, backarc, or arc settings and has an estimated mass of 9 x 10 6 t. This deposit may be of the Kuroko-type. The discovery of the Sunrise deposit in 1997 gives hope that other, similarly large, sulfide deposits may be found in other caldera along the Izu-Bonin Arc. The geological variability along the arc, the high seismicity, the occurrence of active volcanism and submarine hydrothermal venting, and a proven submarine hydrothermal mineral potential coupled with the proximity of the region to Japan suggest that the Izu-Bonin Arc could profitably serve as a natural laboratory for the long-term monitoring of the seafloor. 相似文献
20.
在对CA海山玄武岩CAD21样品岩相学研究基础上,运用电子探针和X-荧光光谱法(XRF)对中太平洋CA海山斜长石斑晶中的环带、斜长石微晶和玄武岩中的硅酸盐进行了化学成分研究。CA海山玄武岩为地幔柱成因的板内玄武岩;斜长石斑晶具有环带结构,环带核部与边部为不连续消光,是不连续环带;环带核部为培长石,边部为拉长石,是岩浆演化过程中形成的正环带,其成因受岩浆演化过程中熔体组分及温、压条件的共同制约。斜长石斑晶核部、边部及斜长石微晶估算温度平均值分别为1 281,1 198和1 071 ℃,分别代表了岩浆源区、岩浆房及岩浆喷发温度,三者温度差值较小,这和洋岛玄武质岩浆的形成及喷发特点相吻合。 相似文献