Fluid Inclusions and Hydrogen,Oxygen, Sulfur Isotopes of Nuri Cu‐W‐Mo Deposit in the Southern Gangdese,Tibet

The Nuri Cu‐W‐Mo deposit is located in the southern subzone of the Cenozoic Gangdese Cu‐Mo metallogenic belt. The intrusive rocks exposed in the Nuri ore district consist of quartz diorite, granodiorite, monzogranite, granite porphyry, quartz diorite porphyrite and granodiorite porphyry, all of which intrude in the Cretaceous strata of the Bima Group. Owing to the intense metasomatism and hydrothermal alteration, carbonate rocks of the Bima Group form stratiform skarn and hornfels. The mineralization at the Nuri deposit is dominated by skarn, quartz vein and porphyry type. Ore minerals are chalcopyrite, pyrite, molybdenite, scheelite, bornite and tetrahedrite, etc. The oxidized orebodies contain malachite and covellite on the surface. The mineralization of the Nuri deposit is divided into skarn stage, retrograde stage, oxide stage, quartz‐polymetallic sulfide stage and quartz‐carbonate stage. Detailed petrographic observation on the fluid inclusions in garnet, scheelite and quartz from the different stages shows that there are four types of primary fluid inclusions: two‐phase aqueous inclusions, daughter mineral‐bearing multiphase inclusions, CO₂‐rich inclusions and single‐phase inclusions. The homogenization temperature of the fluid inclusions are 280°C–386°C (skarn stage), 200°C–340°C (oxide stage), 140°C–375°C (quartz‐polymetallic sulfide stage) and 160°C–280°C (quartz‐carbonate stage), showing a temperature decreasing trend from the skarn stage to the quartz‐carbonate stage. The salinity of the corresponding stages are 2.9%–49.7 wt% (NaCl) equiv., 2.1%–7.2 wt% (NaCl) equiv._, 2.6%–55.8 wt% (NaCl) equiv. and 1.2%–15.3 wt% (NaCl) equiv., respectively. The analyses of CO₂‐rich inclusions suggest that the ore‐forming pressures are 22.1 M Pa–50.4 M Pa, corresponding to the depth of 0.9 km–2.2 km. The Laser Raman spectrum of the inclusions shows the fluid compositions are dominated in H₂O, with some CO₂ and very little CH₄, N₂, etc. δD values of garnet are between ?114.4‰ and ?108.7‰ and δ¹⁸O_H2O between 5.9‰ and 6.7‰; δD of scheelite range from ?103.2‰ to ?101.29‰ and δ¹⁸O_H2O values between 2.17‰ and 4.09‰; δD of quartz between ?110.2‰ and ?92.5‰ and δ¹⁸O_H2O between ?3.5‰ and 4.3‰. The results indicate that the fluid came from a deep magmatic hydrothermal system, and the proportion of meteoric water increased during the migration of original fluid. The δ³⁴S values of sulfides, concentrated in a rage between ?0.32‰ to 2.5‰, show that the sulfur has a homogeneous source with characteristics of magmatic sulfur. The characters of fluid inclusions, combined with hydrogen‐oxygen and sulfur isotopes data, show that the ore‐forming fluids of the Nuri deposit formed by a relatively high temperature, high salinity fluid originated from magma, which mixed with low temperature, low salinity meteoric water during the evolution. The fluid flow through wall carbonate rocks resulted in the formation of layered skarn and generated CO₂ or other gases. During the reaction, the ore‐forming fluid boiled and produced fractures when the pressure exceeded the overburden pressure. Themeteoric water mixed with the ore‐forming fluid along the fractures. The boiling changed the pressure and temperature, oxygen fugacity, physical and chemical conditions of the whole mineralization system. The escape of CO₂ from the fluid by boiling resulted in scheelite precipitation. The fluid mixing and boiling reduced the solubility of metal sulfides and led the precipitation of chalcopyrite, molybdenite, pyrite and other sulfide.     

The relationship between apparent equilibrium temperature and closure temperature with application to oxygen isotope geospeedometry

Oxygen isotope fractionation between coexisting minerals in slowly cooled rocks conveys information about their cooling history. By using the fast grain boundary （FGB） model to simulate closed-system diffusive ex- change of oxygen isotopes between coexisting minerals, I show that the apparent equilibrium temperatures （Tae） by the mineral pair with the largest isotopic fractionation （PLIF） always lies between the closure temperatures （To） of those two minerals. Therefore, when the rate of oxygen diffusion and hence Tc for the PLIF chance to be comparable （such as in the case of quartz and magnetite）, Tae will serve as a good approximation of To regardless of variation in mineral proportions. The specialty of the PLIF in constraining Tac within their Tc range can be generalized to other stable isotope systems and element partitioning. By approximating Tc with Tac and inverting Dodson＇s equation, the cooling rate of plutonic or metamorphic rocks can be inferred.     

白云鄂博碳酸岩墙碳氧同位素地球化学

对内蒙古白云鄂博 REE- Fe- Nb矿床周围碳酸岩墙中共存的方解石和白云石进行了 C和 O同位素分析。结果表明，方解石和白云石的δ 13C值变化范围一致，均为－ 3.5‰～－ 7.3‰，落在正常地幔δ 13C值范围 (－ 5‰± 2‰ )内；而它们的δ 18O值可分为两组，第Ⅰ 组为 9.5‰～ 18.0‰，第Ⅱ 组为 20.6‰～ 22.6‰，均远大于正常地幔δ 18O值范围 (5.7‰± 1.0‰ )。第Ⅰ 组低δ 18O值样品中共存白云石与方解石之间的 C和 O同位素分馏均为负值，因此处于热力学不平衡状态，指示它们自形成后受到过后期热液蚀变，与先前的岩石学观察一致。相反，第Ⅱ 组高δ 18O值样品中白云石与方解石之间的 C和 O同位素分馏均为正值，处于热力学平衡状态，指示它们自形成后未受到后期热液蚀变，因此可能沉淀于晚期低温高δ 18O值流体。第Ⅰ 组碳酸岩墙中白云石的 C和 O同位素组成不呈线性分布，指示碳酸岩浆并非由幔源碳酸盐与沉积碳酸盐混合形成。应用水-岩交换模型计算得到，第Ⅰ 组碳酸岩在侵位后经历了碳酸岩浆期后热液的不均一蚀变，蚀变温度约在 220～ 800℃之间，蚀变流体的 CO2/H2O比值较小 (1/500)，但水 /岩比值变化较大 (10～ 400)。由于低温下方解石与热液之间的碳氧同位素交换速率大于白云石，导致这部分碳酸     

海南福基田幔源辉石结构OH与氢氧同位素

采用IR光谱和质谱技术分析了海南福基田幔源巨晶和包体中辉石的结构羟基红外光谱和氢氧同位素。测试的所有巨晶普通辉石和包体中透辉石及顽火辉石均含结构OH,对比印证了国内外同类矿物的红外光谱特征。结构水质量分数分别是:普通辉石87×10-6~389×10-6;透辉石127×10-6~273×10-6;顽火辉石69×10-6~207×10-6。包体中结构水质量分数为1 811×10-6~5 377×10-6,平均为3 133×10-6。包体中辉石的氢氧同位素特征如下:透辉石的δ(D)为-123.17‰,顽火辉石的δ(D)为-132.04‰;透辉石的δ(18O)为5.96‰,顽火辉石的δ(18O)为5.60‰。实验和对比表明,辉石是海南福基田上地幔重要的"水储库",包体未受地壳成分污染,继承和保持了上地幔"富水贫氘"的特征。上述结果为该地区上地幔研究提供了结构水和氢氧同位素的基础资料。     

海洋天然气水合物氢氧同位素分馏初探

天然气水合物的形成会造成氢、氧同位素的分馏.在实验室合成研究中,利用天然海水 [(含 0.03%十二烷基硫酸钠 (SDS)]与甲烷气体反应,通过对水合物生成前后溶液中的 Cl-的质量浓度和氢、氧同位素组成的测定,研究了天然气水合物生成过程中氢、氧同位素的分馏情况.实验证明氢、氧的重同位素易于富集在水合物中,其在天然海水-甲烷体系中的分馏系数分别为 1.018～ 1.036和 1.003 4～ 1.006 3,这一分馏系数稍大于前人在纯水和 NaCl溶液中所测得的分馏系数.     

川北元坝地区长兴组白云石化作用机制及其对储层形成的影响

通过岩心观察和薄片鉴定,在岩石学和矿物学特征分析基础上,结合白云石有序度测定,碳、氧同位素、锶同位素和稀土元素组成及配分模式分析,详细研究了川北元坝地区长兴组白云石化作用的特征、机制及模式,结果表明长兴组发育微晶白云石(岩)、粉-中晶他形白云石、粉-中晶自形白云石和异形白云石等四种类型,它们的有序度由低变高;白云石的碳、氧同位素、锶同位素和稀土元素组成及配分模式特征表明,长兴组微晶白云石(岩)、粉-中晶他形白云石、粉-中晶自形白云石主要形成于浓缩海水环境、正常海水环境、或者与正常海水相似的地层水环境中,并遭受过热液地质作用的改造,从微晶白云石(岩)→粉-中晶他形白云石→粉-中晶自形白云石是一个沉积埋藏过程中多阶段白云石化作用的产物,异形白云石则由热液作用形成;根据长兴组白云石的矿物学和地球化学特征及白云石化作用与层序和沉积相之间的关系,分别可以用准同生期蒸发泵白云石化作用模式、准同生期渗透回流白云石化作用模式、成岩早期浅埋藏状态下地层水白云石化作用模式和成岩晚期热液白云石化作用模式来解释微晶白云石(岩),粉-中晶他形白云石、粉-中晶自形白云石和异形白云石的形成。白云石化作用是有利于长兴组储层形成的建设性成岩作用。     

猪毛菜在不同降水条件下的水分来源差异研究

通过测定大柴旦与都兰地区猪毛菜木质部水分及其不同潜在水源的稳定性氢氧同位素值,利用多源线性混合模型分析不同水分来源对猪毛菜的贡献率.研究结果表明:大柴旦地区大气降水线为y=7.565x+4.796(R²=0.908),都兰地区大气降水线为y=6.005x-7.856(R²=0.7391),说明两个地区都存在较强的蒸发作用.但是,都兰地区较大柴旦风速大,温度高,雨水蒸发速度快,造成雨水δ¹⁸O偏高,形成比大柴旦地区斜率更小的当地大气降水线.大柴旦和都兰地区的猪毛菜,在两个样地的用水策略上存在显著差异.在降水较少的大柴旦地区,猪毛菜以土壤水为主要水源.在降水较多的都兰地区,则以降水为主要水源.就其对土壤水的使用情况来看,大柴旦的猪毛菜多利用深层土壤水,而都兰地区的猪毛菜却对表层土壤水利用比例较大.两地猪毛菜在生长季的不同时期都存在对利用水源的转换现象.为适应不同地区降水量的变化,猪毛菜根据不同水源调节利用比例.降水格局的改变将导致猪毛菜的水分利用策略发生适应性的变化.     

甘肃马坞金矿成矿流体特征及地质意义

位于西秦岭岷(县)—礼(县)成矿带西段的马坞金矿床,是近年发现的一个中型卡林型金矿床。矿体产出受NWW向断裂构造控制,其赋矿围岩为中泥盆统的千枚岩与灰岩。矿床流体包裹体研究表明,脉石矿物中主要发育CO2-H2O型和H2O溶液型包裹体;均一温度为135~389℃,盐度为4.4%~15.9%,为中-低温、中-低盐度流体;流体成矿压力为34.6~219.8 MPa,成矿深度为1.3~8.1 km。流体包裹体气相成分以H2O、N2为主,其次为CO2、O2,并含有少量CH4、CO等还原性气体;液相成分中阳离子以Ca2+、Na+为主,阴离子以Cl-和SO42-占主导地位,成矿流体为N2-H2O-Ca2+-Cl-体系。氢氧同位素测试结果表明,成矿流体的δ18O水为5.3‰~10.5‰,δD为-123‰~-93‰,成矿流体主要为热卤水。从流体性质及其演化来看,构造体制的转换使流体稳定体系发生改变与沸腾作用是造成金富集成矿的主要因素。     

北麓河多年冻土区降水及河水稳定同位素特征分析

为了进一步全面理解和探索青藏高原水文水循环过程,采用同位素方法并结合气象资料对青藏高原北麓河区域2011年6~12月降水和河水稳定同位素时空特征进行分析。探讨了北麓河降水同位素与日平均气温、降水量之间的相互关系,同时也对比分析了北麓河降水和河水的同位素变化特征。结果表明:北麓河降水同位素在整个观测期内总体受温度控制,但存在季节变化,其中6~9月降水同位素受到温度和降水量效应的共同控制,9月以后则主要受温度的影响。河水同位素与降水同位素相似的变化特征,体现了降水补给特征,另外降水量也能够影响河水同位素变化:降水量小则降水对其影响较小,反之则大。与北麓河降水线相比,河水δ18O~δD关系的斜率和截距偏大,揭示该区域河水除了受大气降水的补给外,还受到区域水体内循环和蒸发分馏作用的影响。     

三峡大坝下游溶解氧变化特性及影响因素分析

根据三峡工程坝区水域实测数据,分析了水库蓄水以后大坝上、下游断面溶解氧浓度和溶解氧饱和度的变化特性,探讨了水位、流量因素对大坝下游水体溶解氧量的影响。结果表明,坝身孔口过流水体大量掺气后进入下游河道导致下游水体溶解氧浓度和饱和度显著增加,甚至达到超饱和状态。由于电站过流基本不改变水体溶解氧量,在电站和坝身孔口同时过流时,两种水体掺混后,下游溶解氧量主要受流量比的影响。此外,下游溶解氧量随流量的增加和下游水位的升高而增大。过坝总流量超过35 000 m3/s,下游水位超过68 m以及坝身孔口过流流量占总流量的绝大部分时,需特别重视溶解氧超饱和现象对水生生物可能造成的影响。