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111.
ZHANGYongbei WANGGuilan NIEJianfeng ZHAOChongshun XUChengyan QIUJiaxiang WangHao 《《地质学报》英文版》2003,77(2):204-211
The Mesoproterozoic Kunyang rift, which is located on the western margin of the Yangtze platform and the southern section of the Kangdian axis, is a rare massive Precambrian iron-copper polymetallic mineralization zone in China. The Mesoproterozoic Wulu (Wuding-Lufeng) basin in the middle of the rift is an elliptic basin controlled by a ring fracture system. Moreover, volcanic activities in the basin display zonation of an outer ring, a middle ring and an inner ring with carbonatitic volcanic rocks and sub-volcanic dykes discovered in the outer and middle rings. The Sm-Nd isochron ages have been determined for the outer-ring carbonatitic lavas (1685 Ma) and basaltic porphyrite of the radiating dyke swarm (1645 Ma) and the Rb-Sr isochron ages for the out-ring carbonatitic lavas (893 Ma) and the middle-ring dykes (1048 Ma). In combination of the U-Pb concordant ages of zircon (1743 Ma) in trachy-andesite of the corresponding period and stratum (1569 Ma) of the Etouchang Formation, as well as the Rb-Sr iso 相似文献
112.
新疆富蕴县蒙库铁矿床地质特征及成因分析 总被引:20,自引:0,他引:20
蒙库铁矿床位于西伯利亚板块的阿尔泰活动陆缘麦兹晚古生代陆内裂谷盆地,并产于该盆地北东缘的中部,即麦兹倒转紧闭复式向斜的北东倒转翼中部.容矿地层为下泥盆统康布铁堡组的下亚组,铁矿体严格受NIⅣ走向的铁木下尔滚次级紧闭向斜构造控制,并产于向斜构造的核部.控矿断层可能是由铁木下尔滚次级紧闭向斜和巴寨区域性断裂联合作用产生的次级断裂构造.蒙库铁矿床的赋矿围岩主要为前进区域变质作用产生的角闪更长片麻岩,局部可见断裂混合岩化现象.近矿围岩蚀变甚弱,主要表现为夕卡岩化作用,出现了石榴子石、绿帘石、钙铁辉石、透闪石等夕卡岩矿物.其成因类型属喷流沉积-变质改造-岩浆热液叠加富集型多因复成铁矿床. 相似文献
113.
零价铁去除Cr(Ⅵ)的一系列批实验结果表明:水溶液中发生的氧化还原反应符合准一级反应;对于相同粒度的铁屑(比表面积2.89m^2/g),固液比由05g/100mL增加到2.0g/100mL,Cr(Ⅵ)质量浓度达到排放标准所需反应时间从26.7min降为3.6min;在固液比相同、原水中Cr(Ⅵ)质量浓度不超过30mg/L时,原水质量浓度增大,达到饮用水标准的反应时间增加;其他条件相同,升高温度可提高零价铁与Cr(Ⅵ)的反应速率。 相似文献
114.
利用核磁共振方法研究水文地质问题及应用实例 总被引:14,自引:1,他引:14
地面核磁共振找水方法是目前唯一直接找水的物探新方法。本文在介绍NMR方法原理的基础上,结合NMR方法技术特点和在中国的应用实例,论述了NMR方法在探测地下水、地下水资源评价等方面的效果,并提出了进一步开展新方法的工作建议。 相似文献
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The activity of Convention at Montserrat Soufrière Hills Volcano, Montserrat, during the period 1995–1999 included numerous violent explosions. Two major cycles of Vulcanian explosions occurred in 1997: a first of 13 explosions between 4 and 12 August and a second of 75 between 22 September and 21 October. The explosions were short-lived events lasting a few tens of seconds during which partial fountain collapse generated pyroclastic surges and pyroclastic flows, and buoyant plumes ascended 3–15 km into the atmosphere. Each explosion discharged on average 3×105 m3 (dense-rock equivalent, DRE) of magma, draining the conduit to depths of 1–2 km. The paper focuses on the first few seconds of three explosions of the 75 that occurred in September/October 1997: 6 October 1997 at 17:50, 7 October 1997 at 16:02 and 9 October 1997 at 12:32. Physical parameters such as exit velocities, magmatic water contents and magma pressures at fragmentation are estimated by following and modelling the ascent of individual momentum-dominated finger jets visible on videos during the initial stages of each explosion. The model treats each finger jet as an incompressible flow sustained by a steady flux of gas and particles during the few seconds of ascent, and produces results that compare favourably with those using a multiphase compressible code run using similar eruptive parameters. Each explosion reveals a progressive increase in eruptive intensity with time, jet exit velocities increasing from 40 m s–1 at the beginning of the explosion up to 140 m s–1 after a few seconds. Modelling suggests that the first magma to exit was largely degassed, whereas that discharged after a few seconds contained up to 2 wt% water. Magma overpressures up to ~10 MPa are estimated to have existed in the conduit immediately prior to each explosion. Progressive increases in jet exit velocity with time over the first few seconds of each explosion provide direct evidence for strong pre-eruptive gradients in water content and magma pressure in the upper reaches (probably 100–500 m) of the conduit. Fountain collapse occurred during the first 10–20 s of each explosion because the discharging jets had bulk densities up to 100 times that of the atmosphere and were unable to entrain enough air to become buoyant. Such high eruptive densities were due to the presence of partially degassed magma in the conduit.Editorial responsibility: A. Woods 相似文献
118.
119.
Makoto Haruna Takahiro Hanamuro Kaoru Uyeda Hirokazu Fujimaki Hiroshi Ohmoto 《Resource Geology》2003,53(2):75-88
Abstract. The petrography, chemical, fluid inclusion and isotope analyses (O, Rb-Sr) were conducted for the shale samples of the Mount McRae Shale collected from the Tom Price, Newman, and Paraburdoo mines in the Hamersley Basin, Western Australia. The Mount McRae Shale at these mines occurs as a footwall unit of the secondary, hematite-rich iron ores derived from the Brockman Iron Formation, one of the largest banded iron formations (BIFs) in the world. Unusually low contents of Na, Ca, and Sr in the shales suggest that these elements were leached away from the shale after deposition. The δ18 O (SMOW) values fall in the range of + 15.0 to +17.9 per mil and show the positive correlation with calculated quartz/sericite ratios of the shale samples. This suggests that the oxygen isotopic compositions of shale samples were homogenized and equilibrated by postdepositional event. The pyrite nodules hosted by shales are often rimmed by thin layers of silica of varying crystallinity. Fluid inclusions in quartz crystals rimming a pyrite nodule show homogenization temperatures ranging from 100 to 240C for 47 inclusions and salinities ranging from 0.4 to 12.3 wt% NaCl equivalent for 18 inclusions. These fluid inclusion data give direct evidence for the hydrothermal activity and are comparable to those of the vein quartz collected from the BIF-derived secondary iron ores (Taylor et al, 2001). The Rb-Sr age for the Mount McRae Shale is 1,952 ± 289 Ma and at least 200 million years younger than the depositional age of the Brockman Iron Formation of ∼ 2.5 Ga in age. All the data obtained in this study are consistent with the suggestion that high temperature hydrothermal fluids were responsible for both the secondary iron ore formation and the alteration of the Mount McRae Shale. 相似文献
120.
根据天气学原理 ,对 11个探空站 1988~ 1997年 7、8、9月逐日 (0 7时、19时 )资料与同期天气系统 (低槽、副热带高压、低压辐合、东风波、台风低压、大陆高压、台风外围 )进行计算与分析 ,结果表明 ,江西省 1988~ 1997年 7~ 9月平均水汽量值为 4 .4 6 g·cm-2 ,其中 :0 7时为 4 .4 4 g·cm-2 ,19时为 4 .4 7g·cm-2 ,7、8、9月平均水汽量值各为4 .8g·cm-2 、4 .6 4 g·cm-2 、4 .0 9g·cm-2 。水汽量分布为南部高北部低 ,东部和西部居中。东风波影响时水汽量最大 ,值为 9.2 3g·cm-2 ,大陆高压影响时水汽量最小 ,值为 0 .78g·cm-2 。轻度干旱频率区水汽量值最大 ,为4 .81g·cm-2 ,最小值出现在重度干旱频率区 ,为 0 .72 g·cm-2 。夏季水汽交换次数为 9.4次 /月 ,水汽更新率为 10 .2天。 相似文献