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1.
利用"freedrift"开放反应系统,研究人工海水中近沉淀平衡状态时二氧化碳分压(p(CO2))的变化对方解石、文石沉淀速率及其动力学方程的影响.反应在恒定的温度(25.0℃±0.2℃)、p(CO2)环境下进行,通过实验得到了不同p(CO2)环境下,方解石和丈石的沉淀速率及动力学方程.研究发现:(1)晶体类型和碳酸盐...  相似文献   

2.
南海东北部海区碳酸钙的饱和面、溶跃面和补偿深度   总被引:2,自引:0,他引:2  
南海东北部碳酸钙地球化学研究得出:上层海水中方解石饱和度450—550%,文石饱和度250—350%.300m以深下层海水方解石与文石饱和度和深度的对数直线相关.深层水中二氧化碳含量0.03mmo1·dm~-3,碳酸根含量0.094mmol·dm~(-3),碳酸氢根含量2.35mmol·dm~(-3)总二氧化碳2.48mmo1·dm~(-3);方解石的饱和面1630m,溶跃面3000m,补偿深度4600m,文石饱和面435m,补偿深度1000m.  相似文献   

3.
利用free-drift开放反应系统,在恒压力(1×105Pa)、恒温度(25.0℃±0.2℃)环境下,研究人工海水中近溶解、沉淀平衡状态时二氧化碳分压(pCO2)的变化对文石溶解、沉淀速率及其动力学方程的影响。每组实验中通入混合气体的pCO2分别为2300×10-6和320×10-6两种,并保持通入气体的pCO2恒定,通过实验得到了这两种pCO2环境下,文石的溶解和沉淀速率及动力学方程。研究结果表明:(1)文石在近溶解、沉淀平衡附近,溶解速率相对于Ac(碳酸盐碱度值)或?(饱和度)的变化速率要大于沉淀速率相对于Ac或?的变化速率;(2)Ac相同时,pCO2越高,溶解速率越高,沉淀速率越低;?相同时,亦是如此;(3)溶解实验中,在?0.8的区间内,反应液和混合气体之间pCO2平衡,反应级数n介于9~10之间;沉淀实验中,文石的反应级数介于2.0~3.2之间。  相似文献   

4.
莱州湾南岸平原地下水化学特征研究   总被引:2,自引:0,他引:2  
用2009年莱州湾南岸地下水最新监测数据,将研究区地下水淡水区、微咸水区、咸盐水区和卤水区进行经典统计分析、相关分析、等值线图和Piper三线图绘制,阐述了水化学类型和成分特征从南往北的变化:EC、TDS、Na+、K+、Mg2+、Cl-、SO42-的平均浓度从南部淡水到北部卤水呈现逐渐增大趋势,因为在卤水区普遍发生碳酸钙沉淀,Ca2+和HCO3-则在咸盐水区浓度达最高;pH值从淡水到卤水呈现从弱碱性到弱酸性的转变;从淡水区向卤水区地下水化学组分阴离子由HCO3-为主变为Cl-为主,阳离子由Ca2+为主变为Na+为主;此外河流对地下水起到淡化和冲刷的作用。主成分分析法提取了水化学3个主成分,分别代表了地下水盐化指标、生物化学作用和碳酸钙沉淀。进一步结合系数比值法和饱和指数计算,在对本区水文、地质以及离子水文地球化学特性分析基础上,指出地下卤水阴阳离子中占绝对优势的Cl-、SO42-、Na+、Mg2+的毫克当量百分数与正常海水的值非常相近而与地下淡水的值相差甚远,反映出本区地下卤水起源于古海水,为沉积海水。此外卤水绝非海水简单浓缩的产物,其间还包括复杂的水化学变质过程及后期演化如矿物沉淀、阳离子交换(K+-Ca2+;Na+-Ca2)+、去白云岩化作用和硅酸盐蚀变等。饱和指数的计算表明石膏在卤水矿化度达100 g/L之后才开始缓慢沉淀,而文石、方解石和白云石基本一直处于饱和沉淀状态,且文石和方解石的饱和指数散点分布极为相似,说明两者可能同时发生沉淀。  相似文献   

5.
国际大洋发现计划(International Ocean Discovery Program, IODP)349航次在南海东部次海盆和西南次海盆残留扩张脊附近的U1431和U1433站位首次钻取基底玄武岩,通过对16块基底玄武岩内的碳酸盐岩脉薄片镜下观察以及激光拉曼光谱分析,揭示碳酸盐矿物为方解石和文石,为典型的洋壳低温热液蚀变次生矿物。U1431站位碳酸盐岩脉为独立的方解石脉、文石脉交替出现;而U1433站位则存在方解石脉、文石脉和方解石-文石共生脉三种情况。此外,U1431站位在基底~42.1m处出现了平行的方解石脉和文石脉,揭示U1431存在不同来源热液的多期活动,即可能存在多次或多阶段不同的热液注入。U1431和U1433站位的碳酸岩脉中,文石的矿物集合体形状基本一致,呈块状、纤维状和放射纤维状;而方解石存在差异, U1431的方解石以斑块状、块状、粒状和纤维状出现,而U1433的方解石仅出现块状。U1431站位的碳酸盐岩脉的丰度明显高于U1433站位。这些均揭示U1431站位的低温热液活动强,而U1433站位则相对弱。两个站位的热液活动不同很可能是由于区域地质环境的差异造成——U1431附近的巨大海山为其提供了热液补给,而U1433远离热液的补给/渗漏点。  相似文献   

6.
国际大洋发现计划(International Ocean Discovery Program, IODP)349航次在南海东部次海盆和西南次海盆残留扩张脊附近的U1431和U1433站位首次钻取基底玄武岩, 通过对16块基底玄武岩内的碳酸盐岩脉薄片镜下观察以及激光拉曼光谱分析, 揭示碳酸盐矿物为方解石和文石, 为典型的洋壳低温热液蚀变次生矿物。U1431站位碳酸盐岩脉为独立的方解石脉、文石脉交替出现; 而U1433站位则存在方解石脉、文石脉和方解石-文石共生脉三种情况。此外, U1431站位在基底~42.1m处出现了平行的方解石脉和文石脉, 揭示U1431存在不同来源热液的多期活动, 即可能存在多次或多阶段不同的热液注入。U1431和U1433站位的碳酸岩脉中, 文石的矿物集合体形状基本一致, 呈块状、纤维状和放射纤维状; 而方解石存在差异, U1431的方解石以斑块状、块状、粒状和纤维状出现, 而U1433的方解石仅出现块状。U1431站位的碳酸盐岩脉的丰度明显高于U1433站位。这些均揭示U1431站位的低温热液活动强, 而U1433站位则相对弱。两个站位的热液活动不同很可能是由于区域地质环境的差异造成——U1431附近的巨大海山为其提供了热液补给, 而U1433远离热液的补给/渗漏点。  相似文献   

7.
瞿成利  刘刚  路波 《海洋科学》2009,33(7):23-29
采用稳定加液一反应系统对5、15和25 ° C下镁方解石沉淀在海水中的形成过程进行了研究.结果表明镁方解石的沉淀速率(R)对过饱和度(Ω)的响应均可通过R=k(Ω-1)°或Log(R)=nLog(Ω-1)+Log(k)形式的动力学方程加以表达.pCO2的变化会显著改变过饱和度进而影响到镁方解石沉淀速率,但这一变化并不会对镁方解石沉淀形成过程的动力学表达产生影响.相比之下,不同温度下镁方解石沉淀形成的动力学方程存在明显差异,表明这一动力学过程同时还具有强烈的热力学相关性.  相似文献   

8.
本文结合已报道的U,Th分离方法和~(231)Pa分离条件建立了Th-Pa-U联合分离流程和测试技术,并用以分离测定一个锰结核和一个深海沉积物样品中的~(231)Pa,U和Th同位素含量的深度分布。用~(231)pa_(ex),~(230)Th_(ex)和~(230)Th_(ex)/~(232)Th法分别计算该锰结核的生长速率为1.5,0.9和1.5mm/Ma。U,Th和~(231)Pa的化学回收率(%)分别为40—80,80—92和60—86。  相似文献   

9.
通过溶液化学平衡反应模型理论计算表明:软泥水和底层海水除Fe在软泥水中呈高价态的分子化合物(Fe(OH)3)和络合离子(Fe(OH)2+),以及二者均存在含量甚微的单一离子Fe3+以外,Fe的其它组分形式和Mn、Cu、Ni、Co元素均以低价态的单一离子、络合离子和分子化合物形式存在。软泥水比底层海水的组分存在形式要多,且组分含量变化幅度要大。软泥水中Fe主要含量是Fe(OH)3,而底层海水主要是Fe2+。软泥水现代正在发生沉析的矿物有:赤铁矿、针铁矿和石英,在外陆架—陆坡海域软泥水可生成方解石、文石,陆坡海域的软泥水还可沉析菱锰矿和水锰矿;底层海水正在沉析的仅是方解石、文石、赤铁矿和针铁矿。碳酸盐类矿物的沉析与海底分布的钙质粘土、泥等沉积物相吻合。水锰矿的生成为陆坡海山区存在的多金属结壳(核)提供了成矿信息,并表明多金属结壳(核)不是通过海水的物理化学作用的途径生成的。  相似文献   

10.
质谱同位素稀释法同时测定海水中痕量铀和钍   总被引:1,自引:0,他引:1       下载免费PDF全文
孟宪厚  黄达峰  宋新 《海洋学报》1985,7(6):728-732
取水样10l,用0.45μm滤膜过滤,加入适量235U和230Th稀释剂,以Fe(OH)3沉淀载带法富集U,Th,进而在CL 5209型萃淋树脂柱上完成U、Th及Fe的分离,并在同一条样品带上完成U和Th的质谱测定,方法的检出限是2.4×109g钍和1.1×10-8g铀,测定海水中铀和钍的精密度分别为±1.7%和±3.6%。  相似文献   

11.
Dissolved and particulate manganese in seawater samples derived from the English Channel has been analyzed using graphite furnace atomic absorption (GFAAS), and inductively coupled plasma atomic emission (ICP—AES) spectroscopies. Because of the high contents of carbonate minerals found in the suspended matter samples, the English Channel constitutes an ideal field area for the study of the Mn2+/Ca2+/CaCO3 system. Owing to the chemical speciation of particulate manganese and the combined use of the X-ray diffraction and electron spin resonance spectroscopy we have shown the importance of the carbonate phase in the stabilization of manganese (II). This has been confirmed by p-pH measurements in the field. All these studies have also indicated that: (1) manganese is associated with calcite in the form of a solid solution, MnxCa1−xCO3; and (2) significant increases in the concentrations of particulate manganese, especially in offshore waters, occur in summer. This seasonal phenomenon has been attributed to the proliferation of coccolithophorids, which are known to be covered with calcified skeletons at high specific surface areas. To appraise the implication of the coccolithophorid-blooms phenomenon on the Mn2+/Ca2+/CaCO3 system, we have used the manganese distribution coefficient, Di, between the liquid phase and CaCO3 particles. Overall we have shown that: (1) Di in summer (i.e. when coccoliths considered as very fine-grained calcite are abundant) is much higher than that obtained in winter; and (2) in the vicinity of the French coast, Di does not vary significantly even in summer. This is because of the high content of chalk-derived particles found in the near-shore waters.  相似文献   

12.
An 8.5 m long apparently undisturbed core from a hilltop on the crest of the East Pacific Rise has uranium and thorium isotope distributions that are very unusual. The core is very poor in 232Th, and very rich in U, particularly at the 500-cm level, where a value of about 150 ppm is reached. At the same depth the 230Thxs reaches very large negative values. These facts could be accounted for if one assumes that solutions rich in U and poor in Th had been postdepositionally injected into the sediments about 90,000–110,000 years ago. The top of the sediment received much of its U from seawater, judging from the 234U238U ratio. Possibly carbonate rich solutions were the carriers of the injected uranium.  相似文献   

13.
The distribution coefficient (λMg) of Mg2+ ions between calcite and solution was found to be 0.012 ± 0.001 (10°C), 0.014 ± 0.001 (15°C), 0.019 ± 0.001 (25°C), 0.024 ± 0.001 (30°C), 0.027 ± 0.001 (35°C) and 0.040 + 0.003 (50°C). This indicates a remarkable dependence on temperature. The effect of the Mg2+/Ca2+ molar ratio in a parent solution on λMg for calcite is small, where the molar ratio lies in the range 0.04-2. However, the λMg value for aragonite tends to decrease with increasing Mg2+/Ca2+ ratio in the parent solution. The largest Mg content of calcite in the Ca(HCO3)2-Mg2+ → calcite system is around 2 mol% in the temperature range 10–50°C. Neither homogeneous nor heterogeneous distribution laws hold for aragonite precipitation, and the temperature effect on the coprecipitation of Mg2+ ions with aragonite is very small.  相似文献   

14.
The saturation of calcite and aragonite in the Arctic Ocean   总被引:1,自引:0,他引:1  
We report on the chemical saturation of CaCO3 in the waters of the Arctic Ocean calculated from total alkalinity (AT) and total dissolved inorganic carbon (CT). Data based on four different expeditions are presented: International Arctic Ocean Expedition (IAOE-91), Arctic Ocean Section 94 (AOS94), Polarstern Arctic '96 expedition (ACSYS 96), and Joint Ocean Ice Study 97 (JOIS 97). The results show a lysocline at around 3500 m for aragonite and that most of the Arctic Ocean sea floor lies above the lysocline for calcite. The only anomaly is the low degree of saturation at the shelf break depth in the Canadian Basin seen in the sections of the AOS94 and JOIS 97 cruises, correlated with nutrient maxima and very low O2 concentration, suggesting decomposition of organic matter. The insignificant variability in degree of saturation between the deep waters of the different basins in the Arctic Ocean indicates a very low sedimentation/remineralisation of organic soft matter.  相似文献   

15.
The apparent solubility product of aragonite in 32‰ seawater at 25.0°C is reported as Ksp = (0.869±0.049) × 10?6(mol2kgseawater?2) thus confirming the value of R.A. Berner, 1976 (Am. J. Sci., 276: 713–730). The apparent solubility product ratio for aragonite and calcite is reported as K′aragoniteK′calcite = 2.05 The deviation of this value from the thermodynamic ratio is atttributed to the formation of a stable low Mg-calcite coating on pure calcite in seawater measurements of solubility.  相似文献   

16.
Analyses of the concentration product (Ca2+) × (CO32−) in the pore waters of marine sediments have been used to estimate the apparent solubility products of sedimentary calcite (KSPc) and aragonite (KSPa) in seawater. Regression of the data gives the relation In KPSPc = 1.94 × 10−3 δP − 14.59 The 2°C, 1 atm value of KSPc is, then, 4.61 × 10−7 mol2 l−2. The pressure coefficient yields a at 2°C of −43.8 cm3 atm−1. A single station where aragonite is present in the sediments gives a value of KSPa = 9.2 × 10−7 (4°C, 81 atm). The calcite data are very similar to those determined experimentally by Ingle et al. (1973) for KSPc at 2°C and 1 atm. The calculated is also indistinguishable from the experimental results of Ingle (1975) if is assumed to be independent of pressure.  相似文献   

17.
1. The adsorption action of basic zinc carbonate adsorbent on uranium in natural seawater can be expressed with the following formula of adsorption isotherm:C=k(U*)n = 8.51× 10-1(U*)0.49,where C is the concentration of uranium on adsorbent; U* is content of uranium in natural seawater employed.2. when the quantity of basic zinc carbonate adsorbent (T) is constant, with the increase of natural seawater quantity through the adsorption column (G), also increased are the adsorption content of uranium of the adsorbent (U), the concentration of uranium on the adsorbent (C) and the concentration of residual uranium (C0*) in natural seawater after adsorbing uranium, while the rate of recovery of uranium (R) is decreased. With the increase of (G) the coefficient of distribution (Kd) decreases to a certain value and then a little rises again.  相似文献   

18.
The rare-earth distribution has been determined in five manganese nodules from a range of marine environments. Manganese nodules from Loch Fyne, Scotland, and the Gulf of Aden are characterized by a low absolute abundance of the rare-earth elements and a low Ce/La ratio compared with deep-sea nodules. This difference is interpreted in terms of the diagenetic remobilization of manganese in the high sedimentation regimes leading to the effective fractionation of manganese from the rare-earth elements and the resultant depletion of the rare earths in nodules from these environments. The mechanism of incorporation of the rare-earth elements into manganese nodules is thought to be either the direct adsorption of these elements from seawater or the scavenging of the elements by colloidal iron oxide prior to their incorporation into the authigenic phase of nodules. There appears to be no evidence for the surface transfer of these elements from inorganic detritus into the authigenic phase of nodules as suggested by previous authors. The distribution of U and Th in the nodules is controlled by factors similar to those controlling the rare-earth abundance in nodules. The higher U/Th ratios in nodules from Loch Fyne and the Gulf of Aden is considered to be due to the preferential reduction of UO2(CO3)34? to some lower-valency uranium species such as U3O8 in nodules from less oxidizing environments.  相似文献   

19.
Dissolved and particulate samples were collected to study the distribution of thorium isotopes (234Th, 232Th and 230Th) in the water column of the Indian sector of the Southern Ocean (from 42°S to 47°S and from 60°E to 66°E, north of the Polar Front) during Austral summer 1999. Vertical profiles of excess 230Th (230Thxs) increases linearly with depth in surface water (0–100 m) and a model was applied to estimate a residence time relative to the thorium scavenging (τscav). Low τscav in the Polar Front Zone (PFZ) are found, compared to those estimated in the Subtropical Front Zone (STZ). Changes in particle composition between the PFZ and STZ could influence the 230Thxs scavenging efficiency and explain this difference. An innovative coupling between 234Th and 230Thxs was then used to simultaneously constrain the settling velocities of small (0.6–60 μm) and large (above 60 μm) particles. Although the different hydrological and biogeochemical regimes visited during the ANTARES IV cruise did not explain the spatial variation of sinking velocity estimates, our results indicate that less particles may reach the seafloor north (60 ± 2 m d− 1, station 8) than south of the Agulhas Return Current (119 ± 23 and 130 ± 5 m d− 1 at stations 3 and 7, respectively). This information is essential for understanding particle transport and by extension, carbon export. In the deep water column, the 230Thxs concentrations did not increase linearly with depth, probably due to lateral transport of North Atlantic Deep Water (NADW) from the Atlantic to the Indian sector, which renews the deep waters and decreases the 230Thxs concentrations. A specific 230Thxs transport model is applied in the deep water column and allows us to assess a “travel time” of NADW ranging from 2 to 15 years.  相似文献   

20.
The coprecipitation of uranium with calcium carbonate   总被引:1,自引:0,他引:1  
This report is one of the studies on the factors controlling the trace element contents of marine calcareous skeletons. The values of the distribution coefficients of UO2 2+ between solutions and carbonate precipitates were measured in the laboratory at 20±1C. From the determination of the uranium contents of marine calcareous skeletons and sea water, the values of uranium between marine calcareous skeletons and sea water are expected as 1.2 to 0.3 for aragonite and 0.2 to 0,0n for calcite. The experimentally measured value of the distribution coefficient for aragonite is thermodynamically discussed. And it was known that the value of the distribution coefficient of UO2 2+ is controlled greatly by the activity coefficient of uranium dissolved in a parent medium and the crystal form of CaCO3. The activity coefficient of uranium in solution mainly owes to the formation of complexes between UO2 2+ and CO3 2–in the solution.  相似文献   

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