Structural and metamorphic controls on the distribution of zircon in an evolving quartzofeldspathic migmatite: an example from the Reynolds Range, central Australia

Three types of zircon occur in a complexly deformed and variably migmatized quartzofeldspathic gneiss from the Reynolds Range, central Australia. The oldest type is inherited from the granitic precursor of the gneiss, and is overgrown by a second group of zircon grains that formed during prograde, granulite facies metamorphism. Partial melting of the gneiss resulted in solution of both the inherited and metamorphic zircon. No new zircon growth accompanied crystallization of the partial melt, suggesting loss of zirconium–rich residual fluids. Hydrous, amphibolite facies retrogression of the gneiss and its migmatized variants during late shearing produced new, idiomorphic zircon in both the shear zone and its wall rocks.
Important implications of this study are that (i) zircon has a tendency to dissolve if it comes into direct contact with a melt produced from anhydrous biotite breakdown in a quartzofeldspathic granulite, (ii) melt crystallization is not necessarily accompanied by zircon growth, and (iii) euhedral zircon can grow from a hydrous fluid phase under subsolidus, amphibolite facies conditions, e.g. within shear zones.     

Contact Partial Melting of Granitic Country Rock, Melt Segregation, and Re-injection as Dikes into Ferrar Dolerite Sills, McMurdo Dry Valleys, Antarctica

Numerous, interconnected, granitic dikes (<30 cm in widthand hundeds of meters in length) cut Ferrar dolerite sills ofthe McMurdo Dry Valleys, Antarctica. The source of the graniticdikes is partial melting of granitic country rock, which tookplace in the crust at a depth of about 2–3 km adjacentto contacts with dolerite sills. Sustained flow of doleriticmagma through the sill generated a partial melting front thatpropagated into the granitic country rock. Granitic partialmelts segregated and collected at the contact in a melt-rich,nearly crystal-free reservoir adjacent to the initial doleritechilled margin. This dolerite chilled margin was subsequentlyfractured open in the fashion of a trapdoor by the graniticmelt, evacuating the reservoir to form an extensive complexof granitic dikes within the dolerite sills. At the time ofdike injection the dolerite was nearly solidified. Unusuallycomplete exposures allow the full physical and chemical processesof partial melting, segregation, and dike formation to be examinedin great detail. The compositions of the granitic dikes andthe textures of partially melted granitic wall rock suggestthat partial melting was characterized by disequilibrium mineraldissolution of dominantly quartz and alkali feldspar ratherthan by equilibrium melting. It is also unlikely that meltingoccurred under water-saturated conditions. The protolith granitecontains only 7 vol.% biotite and estimated contact temperaturesof 900–950°C suggest that melting was possible ina dry system. Granite partial melting, under closed conditions,extended tens of meters away from the dolerite sill, yet meltsegregation occurred only over less than one-half a meter fromthe dolerite chilled margin where the degree of partial meltingwas of the order of 50 vol.%. This segregation distance is consistentwith calculated length scales expected in a compaction-drivenprocess. We suggest that the driving force for compaction wasdifferential stress generated by a combination of volume expansionas a result of granite partial melting, contraction during doleritesolidification, and relaxation of the overpressure driving doleriteemplacement. On a purely chemical basis, the extent of meltsegregation necessary under fractional and batch melting tomatch the Rb concentrations between melt and parent rock isa maximum of 48 and 83 vol.% melt, respectively. KEY WORDS: Antarctica; dike injection; disequilibrium; granite partial melting; silicic melt segregation     

Geochronology,Petrogenesis and Tectonic Setting of the Late Jurassic I-type Granites in the North Qinling Orogenic Belt,Central China

The North Qinling Orogenic Belt(NQOB) is a composite orogenic belt in central China. It started evolving during the Meso–Neoproterozoic period and underwent multiple stages of plate subduction and collision before entering intra-continental orogeny in the Late Triassic. The Meso–Cenozoic intra-continental orogeny and tectonic evolution had different responses in various terranes of the belt, with the tectonic evolution of the middle part of the belt being particularly controversial. The granites...     

地球早期大陆地壳的形成与演化

现代地球岩石圈主要由镁铁质上地幔和长英质地壳两个储集层组成,研究大陆地壳的形成和演化对揭示地球早期地质过程和物质循环、厘定板块构造启动时限具有重要意义。冥古宙—始太古代具有更高的地幔潜能温度和地温梯度,岩浆海冷却形成薄的原始地壳;大洋岩石圈表现为韧性,主要构造机制应为停滞盖层模式,有地幔柱参与。太古宙片麻岩中奥长花岗岩—英云闪长岩—花岗闪长岩(TTG)的出现标志着镁铁质原始地壳向长英质陆壳转变的开始。本文总结了地球早期停滞盖层模式到现代板块构造模式下含水玄武岩部分熔融、结晶分异形成大陆地壳的过程,主要包含幔源岩浆停滞盖层(“自下而上”的热管火山岩和“自上而下”的深成侵入岩构造模式)、增厚镁铁质地壳部分熔融、俯冲洋壳、岛弧及洋底高原部分熔融模式;陆壳的破坏和消减主要受陨石撞击、分层沉降、重力不稳导致拆沉控制;板块构造的出现进一步促进了地球内部的热量扩散,俯冲作用加快了洋壳和陆壳之间的物质循环。最后,结合太古宙变质岩、古老克拉通岩石学特征和锆石Hf、O及全岩Nd、Sr、Ar、Ti同位素组成,讨论了陆壳的形成时间和演化过程：3.0 Ga之前形成了现有陆壳体积的60%～70%,厚度约为20～4...     

东昆仑拉陵高里河沟脑地区晚三叠世花岗闪长斑岩年代学、岩石地球化学及Hf同位素特征

本文对东昆仑拉陵高里河沟脑花岗闪长斑岩开展详细的全岩地球化学、LA- ICP- MS锆石U- Pb年代学、锆石Hf同位素研究,确定其形成时代,并探讨其岩石成因及成岩构造背景。结果显示,花岗闪长斑岩LA- ICP- MS锆石U- Pb年龄为231. 1±1. 2 Ma,指示其侵位于晚三叠世早期。全岩K2O/Na2O值为0. 69～0. 71,Mg#值为40. 5～41. 6,里特曼指数σ为1. 90～2. 09,A/CNK=1. 01～1. 03,属弱过铝质中—高钾钙碱性岩石系列。岩石的轻重稀土元素分异明显,(La/Yb)N值为19. 54～25. 52,具弱负Eu异常（δEu为0. 96～0. 97）,富集大离子亲石元素K、Rb、Ba、Th,亏损高场强元素Nb、Ta、Ti等,具有高的Sr含量(606. 0×10-6～647. 9×10-6)和Sr/Y值(60. 38～62. 99),较低的Y(9. 62×10-6～10. 66×10-6)和Yb(0. 86-6～0. 92×10-6)含量,显示Adakite（高锶低钇中酸性岩）的地球化学特征。锆石Hf同位素εHf(t)值介于-6. 93~-2. 94,地壳模式年龄（TDM2）范围为1. 45~1. 70 Ga。综合分析表明,拉陵高里河沟脑花岗闪长斑岩形成于东昆仑洋壳俯冲末期至局部碰撞的转换阶段,岩浆源于高压条件下的加厚下地壳部分熔融。     

有关埃达克岩实验应用中几个问题的探讨

实验研究非常重要,是花岗岩(和埃达克岩)理论创新的源泉之一。近年来,国内在埃达克岩实验研究方面取得了很大的成绩。在这个领域,中国在国际上是处于领先水平的,虽然得到的认识并不相同,这是很正常的。本文讨论了与埃达克岩有关的一些实验研究问题,认为:1下地壳底部是缺水的,花岗岩是在缺水条件下部分熔融的,应当慎重对待在饱和水和有水加入情况下的实验结果。2要注意残留相组分中是否有斜长石出现,不能只关注石榴石,石榴石与斜长石配合起来才能得出正确的认识。3 1.0 GPa压力下石榴石出现线的真实含义是什么?它只表明与之平衡的熔体是贫Yb的。但是,贫Yb的花岗岩不只是埃达克岩,喜马拉雅型花岗岩也贫Yb,因此,还需要考虑斜长石消失的情况,如果石榴石出现而斜长石消失了,熔体是埃达克岩;如果石榴石出现而斜长石没有消失,则熔体为喜马拉雅型花岗岩。由于国外没有喜马拉雅型花岗岩的概念,因此,对国外某些在1 GPa条件下得到的实验资料应当仔细鉴别,也许其中有一些熔体并非埃达克岩,而是喜马拉雅型花岗岩。4相变反应不同于部分熔融反应,不能把相变反应的结果解释为部分熔融的结果。相变反应是在温度压力增加的情况下发生的,不是产生花岗岩的主要方式;部分熔融反应主要是在温度增加压力不变的条件下发生的,是产生花岗岩的主要方式。5实验研究得出的一个重要的结论是:与榴辉岩平衡的熔体是埃达克岩,因此,埃达克岩的真谛可能就是非常简单的一句话:源区有石榴石无斜长石。只要符合这个标志,与其平衡的熔体必然是高Sr低Yb的;只要符合这个标志,与其平衡的熔体必然是在较高的压力下形成的。高压可能就是埃达克岩最重要的构造意义。     

典型融雪期雪层融雪水出流条件模拟及分析

融雪期雪层融雪水的运移及流出过程模拟乃是国际冰雪水文学研究的难点之一,准确模拟融雪水的出流过程对于春季融雪型洪水的预报具有重要作用。本研究基于EM50、农业小环境监测仪和一些常规监测手段,获取了典型融雪期雪层的雪粒径、雪深及日气温数据,利用Excel、DPS、Arcgis及SPSS等分析软件对数据进行综合处理,并采用回归分析对融雪水的出流条件进行了建模分析,利用神经网络模型对模拟结果进行检验。结果表明:积温可作为融雪水外流的参考性指标,用于融雪水外流过程的预测分析;雪粒径和雪深都与融雪水外流积温条件存在显著相关性,且相关系数0.96;逐步回归可以很好地模拟融雪水外流的积温条件,模拟的误差仅为124.5℃·min,时间误差为15 min,模拟效果良好。该研究对于进一步探讨融雪期雪层融雪水的出流规律、开展雪层融雪水运移过程的数值模拟等工作具有重要意义。     

基于遥感的土壤电阻率估算研究

以我国长江中下游的南京及其周边15个市(县)为例,采用野外测定、室内分析与遥感反演相结合的方法,开展了土壤电阻率估算研究.选用影响土壤电阻率的土壤水分、土壤温度、土壤可溶盐总量与土壤阳离子交换量等4个主要因子,遥感反演土壤水分和温度空间分布,以获取估算土壤电阻率所需要的主要参数;采用偏最小二乘二次多项式(PLSQM)模型对不同地表覆盖类型下的土壤电阻率进行估算,PLSQM估算模型的估算值与实测值的相关系数达到0.85,平均相对误差(MRE)为19.02%,均方根误差(RMSE)为7.79.结果表明,草地、农田、林地3种不同地表覆盖类型下土壤电阻率有明显差异,PLSQM模型实现了较高估算精度,具有较好的应用潜力.     

Calculation of partial melting equilibria in the system Na2O–CaO–K2O–FeO–MgO–Al2O3–SiO2–H2O (NCKFMASH)

A thermodynamic model for haplogranitic melts in the system Na₂O–CaO–K₂O–Al₂O₃–SiO₂–H₂O (NCKASH) is extended by the addition of FeO and MgO, with the data for the additional end‐members of the liquid incorporated in the Holland & Powell (1998) internally consistent thermodynamic dataset. The resulting dataset, with the software thermocalc , is then used to calculate melting relationships for metapelitic rock compositions. The main forms for this are P–T and T–X pseudosections calculated for particular rock compositions and composition ranges. The relationships in these full‐system pseudosections are controlled by the low‐variance equilibria in subsystems of NCKFMASH. In particular, the solidus relationships are controlled by the solidus relationships in NKASH, and the ferromagnesian mineral relationships are controlled by those in KFMASH. However, calculations in NCKFMASH allow the relationships between the common metapelitic minerals and silicate melt to be determined. In particular, the production of silicate melt and melt loss from such rocks allow observations to be made about the processes involved in producing granulite facies rocks, particularly relating to open‐system behaviour of rocks under high‐grade conditions.     

Effect of climate change on runoff of a glacierized Himalayan basin

The continuous increase in the emission of greenhouse gases has resulted in global warming, and substantial changes in the global climate are expected by the end of the current century. The reductions in mass, volume, area and length of glaciers on the global scale are considered as clear signals of a warmer climate. The increased rate of melting under a warmer climate has resulted in the retreating of glaciers. On the long‐term scale, greater melting of glaciers during the coming years could lead to the depletion of available water resources and influence water flows in rivers. It is also very likely that such changes have occurred in Himalayan glaciers, but might have gone unnoticed or not studied in detail. The water resources of the Himalayan region may also be highly vulnerable to such climate changes, because more than 50% of the water resources of India are located in the various tributaries of the Ganges, Indus and the Brahmaputra river system, which are highly dependent on snow and glacier runoff. In the present study, the snowmelt model SNOWMOD has been used to simulate the melt runoff from a highly glacierized small basin for the summer season. The model simulated the distribution and volume of runoff with reasonably good accuracy. Based on a 2‐year simulation, it is found that, on average, the contributions of glacier melt and rainfall in the total runoff are 87% and 13% respectively. The impact of climate change on the monthly distribution of runoff and total summer runoff has been studied with respect to plausible scenarios of temperature and rainfall, both individually and in combined scenarios. The analysis included six temperature scenarios ranging between 0·5 and 3 °C, and four rainfall scenarios (?10%, ?5%, 5%, 10%). The combined scenarios were generated using temperature and rainfall scenarios. The combined scenarios represented a combination of warmer and drier and a combination of warmer and wetter conditions in the study area. The results indicate that, for the study basin, runoff increased linearly with increase in temperature and rainfall. For a temperature rise of 2 °C, the increase in summer streamflow is computed to be about 28%. Changes in rainfall by ±10% resulted in corresponding changes in streamflow by ±3·5%. For the range of climatic scenarios considered, the changes in runoff are more sensitive to changes in temperature, compared with rainfall, which is likely due to the major contribution of melt water in runoff. Such studies are needed for proper assessment of available water resources under a changing climate in the Himalayan region. Copyright © 2005 John Wiley & Sons, Ltd.