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121.
陈博  朱永峰 《岩石学报》2010,26(8):2287-2298
克拉玛依蛇绿混杂岩带百口泉剖面由尖晶石蛇纹岩、辉长岩、玄武岩和硅质岩组成。岩相学研究表明,百口泉辉长岩分为堆晶岩(具堆晶结构)和辉长岩(具辉长结构)两类,且均经历了低-中级变质改造。微量元素地球化学显示其岩浆起源于亏损地幔,强烈的Sr异常和Eu异常表明强烈的斜长石堆晶过程。根据其稀土配分模式推测其源区为尖晶石相的地幔橄榄岩。结合野外地质关系和地球化学特征,白碱滩尖晶石二辉橄榄岩能够代表其源区成分,利用微量元素模拟其岩浆演化过程显示:尖晶石二辉橄榄岩发生2.5%部分熔融所形成的熔体,通过10%~20%分离结晶可以形成堆晶辉长岩,经过80%~90%分离结晶则可以形成具辉长结构的辉长岩。因此,蛇绿混杂岩中零星分布的堆晶岩和辉长岩团块是同源岩浆演化的产物。对分离结晶过程中Nb元素地球化学行为的研究表明,岩浆的结晶分异能够导致辉长岩明显亏损Nb。  相似文献   
122.
大兴安岭北部塔河花岗杂岩体的地球化学特征及成因   总被引:3,自引:3,他引:0  
张彦龙  赵旭晁  葛文春  张吉衡  高妍 《岩石学报》2010,26(12):3507-3520
塔河杂岩体位于塔源-喜桂图缝合带北侧的额尔古纳地块东部,是早古生代侵入的花岗杂岩体。该杂岩体的主要岩石类型为正长花岗岩、二长花岗岩,少量碱长花岗岩和花岗闪长岩,辉长岩以包体存在于花岗岩中。岩石成因类型为典型的Ⅰ型后造山侵入体。岩体在野外地质特征、矿物组合、显微结构、化学成分及锆石Hf同位素特征等方面都表现出岩浆混合成因。在早古生代额尔古纳地块与兴安地块拼合后的后造山伸展拉张背景下,地壳和地幔都发生部分熔融,直接起源于亏损地幔的玄武质岩浆侵入到下地壳熔融的花岗质岩浆房,经结晶分异作用,形成了塔河杂岩体不同的岩石类型。花岗岩的εHf(t)为-0.8~+5.6之间,Hf模式年龄在0.9~1.5Ga之间,反映塔河花岗岩的源岩应该是在中-新元古代时期由亏损地幔起源的新生地壳物质。结合额尔古纳地块早古生代和中生代花岗岩锆石Hf同位素资料,我们认为额尔古纳地块在中-新元古代时曾发生过一次重要的地壳增生事件。  相似文献   
123.
南京南郊大气湍流统计特征的实验研究   总被引:2,自引:1,他引:1  
利用2011年8月南京南郊溧水大气边界层加强实验站的大气湍流观测资料,分析了城市郊区自然状态下垫面大气湍流宏观统计规律,以及湍流动量、热量、水汽和CO2的湍流输送特征。结果表明:不稳定层结下,3方向风速归一化标准差σu/u*,σv/u*,σw/u*,随稳定度参数ζ呈1/3幂次关系;稳定层结下也呈现类似规律;近中性条件下,分别趋近于常数。不稳定层结下,温度、比湿、CO2质量浓度归一化标准差σT/|T*|,σq/|q*|,σρCO2/|ρCO2*|,随ζ呈1/3幂次负相关关系,但结果相对离散,并且相对离散的数据对应着较小的|T*|、|q*|、|ρCO2*|值;稳定层结下,三者ζ之间的关系没有明显变化规律。实验期间相对于感热通量,潜热通量在热量平衡中所占比例较大;CO2通量平均值为负,整体表现为碳汇。水汽、热量和CO2均存在水平输送。  相似文献   
124.
There are many arguments on energy sources and main controlling factors of geothermal fields, so a systematic study on the distribution of ground temperature fields shall be necessary. In this paper the thermal conduction forward method of geothermal field is used to simulate cooling rate of abnormal heat sources and heat transfer of the paleo-uplift model. Combined with a large number of geothermal field exploration cases and oil exploration well temperature curves of domestic and foreign, the following conclusions are drawn: (1) According to the magmatic activity time, the magmatism activities are divided into two categories: Magma active areas (activity time < 500 000 years) and weak/magma inactive areas (activity time > 500 000 years). The latter has a fast cooling rate (the cooling time of the magma pocket buried around 10 km is less than 200 000 years) after it has intruded into the shallow layer and it has no direct contribution to modern geothermal fields; (2) China belongs to a weak/magma inactive area such as Tengchong region and Qinghai-Tibet region because the chronological data of these regions show that its magma activity time is more than 500 000 years; (3) The temperature of most geothermal fields can be obviously divided into three segments in the vertical direction: A high geothermal gradient segment (Segment H) at the surface, then a low geothermal gradient segment (Segment L) at a secondary depth, and finally a lower temperature segment (Segment D) at a deeper depth. The temperature isoline presents a mirror reflection relation on the temperature profile, indicating that geothermal field is dominated by heat conduction, rather than having an abnormally high temperature “heat source” to provide heat; (4) Near-surface (0-5 km) materials’ lateral heterogeneity caused by tectonic movement shall probably be the main controlling factor of ground temperature fields.  相似文献   
125.
岩浆-热液系统中铁的富集机制探讨   总被引:25,自引:17,他引:8  
与岩浆-热液系统有关的铁矿类型有岩浆型钒钛磁铁矿床、玢岩铁矿、矽卡岩型铁矿和海相火山岩型铁矿,与这些铁矿有关的岩浆岩从基性-超基性、中性到中酸性岩均有,其中岩浆型钒钛磁铁矿床与基性-超基性深成侵入岩有关,形成于岩浆阶段,主要与分离结晶作用有关,但是厚大的富铁矿石的形成则可归结于原始的富铁钛苦橄质岩浆、分离结晶作用、多期次的岩浆补充以及流动分异等联合过程。钒钛磁铁矿石产于岩体下部还是上部与母岩浆的氧逸度有关:高的氧逸度导致磁铁矿早期结晶而使得其堆积于岩体的下部,相反,低氧逸度则导致低品位的浸染状矿石产于岩体的上部。虽然野外一些证据表明,元古宙斜长岩中的磷铁矿石可能是不混溶作用形成的,但是目前尚无实验证据。某些玢岩铁矿的一些磷灰石-磁铁矿石可能与闪长质岩浆同化混染了地壳中的磷导致的不混溶作用有关。除此之外,其他各类与岩浆作用有关的铁矿床均与岩浆后期的岩浆-热液作用有关。这些不同类型铁矿床的蚀变和矿化过程具有相似性,反映了它们形成过程具有相似的物理化学条件。成矿实验以及流体包裹体研究表明,岩浆-流体转换过程中出溶流体的数量以及成分受多种因素控制,其中岩浆分离结晶作用以及碳酸盐地层和膏盐层的混染可导致出溶的流体中Cl浓度的升高。早期高氧逸度环境可以使得硫以SO42-形式存在,抑制硫与铁的结合形成黄铁矿,有利于铁在早期以Cl的络合物发生迁移。大型富铁矿的形成需要一个长期稳定的流体对流循环系统,而岩浆的多期侵位或岩浆房以及在相对封闭的环境中(需要一个不透水层)一个有利于流体循环的断裂/裂隙系统是形成一个长期稳定的流体对流循环系统的必要条件。但是由于不同地质环境,流体中铁的卸载方式和位置会有明显差别,由此导致不同的矿石结构构造和不同的矿体产状。  相似文献   
126.
Soil heat flux is important for surface energy balance (SEB), and inaccurate estimation of soil heat flux often leads to surface energy imbalance. In this paper, by using observations of surface radiation fluxes and soil temperature gradients at a semi-arid grassland in Xilingguole, Inner Mongolia, China from June to September 2008, the characters of the SEB for the semi-arid grassland were analyzed. Firstly, monthly averaged diurnal variations of SEB components were revealed. A 30-min forward phase displacement of soil heat flux (G) observed by a fluxplate at the depth of 5-cm below the soil surface was conducted and its effect on the SEB was studied. Secondly, the surface soil heat flux (Gs) was computed by using harmonic analysis and the effect of the soil heat storage between the surface and the fluxplate on the SEB was examined. The results show that with the 30-min forward phase displacement of observed G, the slope of the ordinary linear regression (OLR) of turbulent fluxes (H+LE) against available energy (Rn–G) increased from 0.835 to 0.842, i.e., the closure ratio of SEB increased by 0.7%, yet energy imclosure of 15.8% still existed in the SEB. When Gs, instead of G was used in the SEB equation, the slope of corresponding OLR of (H+LE) against (Rn–Gs) reached 0.979, thereby the imclosure ratio of SEB was reduced to only 2.1%.  相似文献   
127.
Large rivers have been previously shown to be vertically heterogeneous in terms of suspended particulate matter (SPM) concentration, as a result of sorting of suspended solids. Therefore, the spatial distribution of suspended sediments within the river section has to be known to assess the riverine sedimentary flux. Numerous studies have focused on the vertical distribution of SPM in a river channel from a theoretical or experimental perspective, but only a few were conducted so far on very large rivers. Moreover, a technique for the prediction of depth‐integrated suspended sediment fluxes in very large rivers based on sediment transport dynamics has not yet been proposed. We sampled river water along depth following several vertical profiles, at four locations on the Amazon River and its main tributaries and at two distinct water stages. Depending on the vertical profile, a one‐ to fivefold increase in SPM concentration is observed from river channel surface to bottom, which has a significant impact on the ‘depth‐averaged’ SPM concentration. For each cross section, a so‐called Rouse profile quantitatively accounts for the trend of SPM concentration increase with depth, and a representative Rouse number can be measured for each cross section. However, the prediction of this Rouse number would require the knowledge of the settling velocity of particles, which is dependent on the state of aggregation affecting particles within the river. We demonstrate that in the Amazon River, particle aggregation significantly influences the Rouse number and renders its determination impossible from grain‐size distribution data obtained in the lab. However, in each cross section, the Rouse profile obtained from the fit of the data can serve as a basis to model, at first order, the SPM concentration at any position in the river cross section. This approach, combined with acoustic Doppler current profiler (ADCP) water velocity transects, allows us to accurately estimate the depth‐integrated instantaneous sediment flux. Copyright © 2010 John Wiley & Sons, Ltd.  相似文献   
128.
129.
 During the 1944 eruption of Vesuvius a sudden change occurred in the dynamics of the eruptive events, linked to variations in magma composition. K-phonotephritic magmas were erupted during the effusive phase and the first lava fountain, whereas the emission of strongly porphyritic K-tephrites took place during the more intense fountain. Melt inclusion compositions (major and volatile elements) highlight that the magmas feeding the eruption underwent differentiation at different pressures. The K-tephritic volatile-rich melts (up to 3 wt.% H2O, 3000 ppm CO2, and 0.55 wt.% Cl) evolved to reach K-phonotephritic compositions by crystallization of diopside and forsteritic olivine at total fluid pressure higher than 300 MPa. These magmas fed a very shallow reservoir. The low-pressure differentiation of the volatile-poor K-phonotephritic magmas (H2O<1 wt.%) involved mixing, open-system degassing, and crystallization of leucite, salite, and plagioclase. The eruption was triggered by intrusion of a volatile-rich magma batch that rose from a depth of 11–22 km into the shallow magma chamber. The first phase of the eruption represents the partial emptying of the shallow reservoir, the top of which is within the volcanic edifice. The newly arrived magma mixed with that resident in the shallow reservoir and forced the transition from the effusive to the lava fountain phase of the eruption. Received: 14 September 1998 / Accepted: 10 January 1999  相似文献   
130.
R. J. Harding  C. R. Lloyd 《水文研究》2008,22(13):2346-2357
Wet grasslands are important both for their conservation value and for their important hydrological function. Evaporation is an important component of the water balance of a wetland. Where water is limited rainfall and/or surface (or sub‐surface) inflows are required to balance the summer evaporation and thus become a significant factor in the maintenance and environmental health of a wetland. This study presents an almost complete year of measurements of the water and energy balance of a wet grassland in the Somerset Levels in southwest England. The majority of the radiant energy at this site goes into evaporation. There is a strong seasonality of the controls on evaporation; the roughness length varies by a factor of 10 between winter and summer. The surface resistance to evaporation is low, close to zero, during the winter when the water table is at, or just below the surface. In the summer the water table drops to 80 cm below the surface; there is no sign of soil water stress on the evaporation but a clear effect of the senescence of grass during seed head production and of the subsequent harvest. There is clear evidence that water for evaporation is provided by the drainage ditches through sub‐surface flow. Standard evaporation formulae—such as the Penman‐Monteith equation with constant and standard parameters—provide a reasonable simulation of the total evaporation at this site, although they miss some of the seasonal detail. Copyright © 2008 John Wiley & Sons, Ltd.  相似文献   
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