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71.
含水矿物在真空下的释Ar机制:Ar-Ar热年代学面临的新问题   总被引:2,自引:0,他引:2  
马芳  穆治国 《地学前缘》2002,9(2):505-510
地质体的实际情况、激光显微探针束研究、XRD和SEM观测以及真空加热下Ar的释放特征都表明体积扩散不是含水矿物在真空加热中释放Ar的唯一机制。在低温下 ,Ar的释放主要受由缺陷引起的短程扩散和体积扩散共同作用的多途径扩散机制制约 ;而在高温下 ,由于含水矿物在真空中不够稳定 ,Ar的释放受到脱羟基、脱氢、氧化反应、分层作用等造成的晶体结构改变的强烈影响。含水矿物在高温下的氧化分解会导致矿物中原始Ar浓度梯度的均一化 ,因而无法得到真实的Ar分布剖面 ,也无法据此计算矿物的封闭温度 ,并进而可能影响到ArAr年龄坪的地质意义。  相似文献   
72.
葡萄状 -雪花状白云岩是白云岩形成之后经淡水淋滤作用而成 ,葡萄内或雪花周围的有机物质不是原生藻 ,而是蓝绿藻经细菌腐解后形成的细菌集合体。该套白云岩的形成与沉积环境关系密切 ,与藻类多少无关。葡萄状白云岩富含有机物质 ,而雪花状白云岩孔洞发育 ,因此葡萄状 -雪花状白云岩既是生油层 ,又是良好的储集层 ,对其重新认识和定位 ,必将为寻找深部油气资源提供极为重要场所  相似文献   
73.
西藏蛇绿岩中二种合金矿物新变种   总被引:5,自引:0,他引:5  
在西藏雅鲁藏布江蛇绿岩带的东部,距拉萨200km的泽当罗莎蛇绿岩的铬铁矿中,发现有种类繁多的合金矿物,铬铁镍矿和依铁镍矿就是其中二种。铬铁镍矿分子式:Ni0.41Fe0.35Cr0.24,为等轴晶系,空间群为Fm3m,晶胞参数a=0.35622(2)nm。铱铁镍矿分子式:Ni0.66Fe0.18Ir0.16,属等轴晶系,空间群Oh^5-Fm3m,晶胞参数a=0.46486(4)mm。  相似文献   
74.
The distribution and partitioning of trace metals (Co, Cu, Fe, Mn, Ni, and Zn) between dissolved and particulate phases were studied in the Tanshui Estuary. The upper reach of the estuary is hypoxic and heavily polluted due to domestic and industrial discharges. The concentration ranges of dissolved and leachable particulate trace metals in the Tanshui Estuary were: Co: 0.3–6.1 nM, 1.8–18.6 mg kg−1; Cu: 5–53 nM, 22–500 mg kg−1; Fe: 388–3,364 nM, 1.08–6.67%; Mn: 57–2,914 nM, 209–1,169 mg kg−1; Ni: 7–310 nM, 6–108 mg kg−1; and Zn: 12–176 nM, 62–1,316 mg kg−1; respectively. The dissolved concentrations of the metals were 2–35 times higher than the average values of the world river water. The distributions of dissolved and particulate studied metals, except Mn, in the estuary showed scattering, which could be attributed to the discharges from many industrial wastewater disposal works located in the upper tributaries. The daily input of dissolved metals from the disposal works to the Tanshui Estuary ranged from 0.1–0.4 tons. Dissolved Mn was nearly conservative in the region with salinity higher than 10 psu, while particulate Mn decreased in the region with salinity of 10–15 psu. The concentration increased significantly seawards, corresponding with the distribution of dissolved oxygen. The distribution coefficient (KD) for Mn in the lower estuary was nearly three orders of magnitude higher than in the upper estuary. This phenomenon may be attributed to the diffusion of Mn from the anoxic sediment in the upper estuary and gradual oxidation into particulate Mn in the middle and lower estuary as the estuarine water became more oxygenated. The distribution coefficient for Cu decreased with increasing salinity. The percentages of trace metals bound by suspended particulate matter decreased in the following order: Fe>Zn, Cu>Co>Mn>Ni.  相似文献   
75.
昆仑山口西8.1级地震在四川地区的前兆异常效应   总被引:2,自引:0,他引:2  
程式  杜方 《四川地震》2002,(4):7-13
对昆仑口西8.1级地震发生前后四川地区地震前兆监测台网的测值曲线进行了系统的清理,发现存在有明显的孕震效应和震时效应,异常效应的幅度很大,容易鉴别,这对人类认识特大地震的影响场很有意义。  相似文献   
76.
Velocity profile of a sand cloud blowing over a gravel surface   总被引:2,自引:0,他引:2  
Particle dynamic analyzer (PDA) measurement technology was used to study the turbulent characteristics and the variation with height of the mean horizontal (in the downwind direction) and vertical (in the upward direction) particle velocity of a sand cloud blowing over a gravel surface. The results show that the mean horizontal particle velocity of the cloud increases with height, while the mean vertical velocity decreases with height. The variation of the mean horizontal velocity with height is, to some extent, similar to the wind profile that increases logarithmically with height in the turbulent boundary layer. The variation of the mean vertical velocity with height is much more complex than that of the mean horizontal velocity. The increase of the resultant mean velocity with height can be expressed by a modified power function. Particle turbulence in the downwind direction decreases with height, while that in the vertical direction is complex. For fine sands (0.2–0.3 mm and 0.3–0.4 mm), there is a tendency for the particle turbulence to increase with height. In the very near-surface layer (<4 mm), the movement of blown sand particles is very complex due to the rebound of particles on the bed and the interparticle collisions in the air. Wind starts to accelerate particle movement about 4 mm from the surface. The initial rebound on the bed and the interparticle collisions in the air have a profound effect on particle movement below that height, where particle concentration is very high and wind velocity is very low.  相似文献   
77.
平原河网区域来水组成原理   总被引:1,自引:0,他引:1  
朱琰  陈方  程文辉 《水文》2003,23(2):21-24
对于一般树状分布河网,上一级河道总是汇入至下一级河道,位于河道下游断面的流量总是由其上游汇集而至。但对于平原河网地区,特别是人工控制建筑物众多,又受潮汐影响的地区(如太湖流域),河网错综复杂,水流方向不定,要跟踪某个断面的水流去向,或某个河段的水体、断面流量是从哪里汇集而来的,非常困难。但这样的问题在生产实践中往往对其很感兴趣。例如从常熟枢纽引长江水流进入望虞河后,流向何处?河网各断面流量中或各河段水体中常熟枢纽引江水量占多少比重?对这些问题的研究可以估计常熟枢纽引江的效果和影响范围。因此,平原河网区域来水组成方法在生产实践中具有重要意义。重点介绍了平原河网区域来水组成原理及其在太湖流域的应用。  相似文献   
78.
数字化气氡观测干扰因素的分析研究   总被引:1,自引:0,他引:1       下载免费PDF全文
在进行地下流体数字化气氡观测及将观测资料应用于震情分析的过程中 ,发现某些干扰因素对数字化气氡观测和水氡的影响不同。在目前所用观测仪器和方法的条件下 ,气温对气氡值的影响系数为 - 0 4 % /℃ ;气压对气氡测值的影响系数为 0 1% /hPa ;不同类型的气水分离装置对气氡观测的影响很显著 ;同一含水层的井 (泉 )出水量的短期变化可引起观测水井流量的变化 ,但对气氡测值影响不显著 ;气氡测值对逸出气流量的变化反映不明显 ;逸出气含有杂质及气路泄漏等均会引起测值的下降。结合仪器的工作原理 ,对干扰产生的机制以及排除的方法进行了讨论  相似文献   
79.
It has been proved through experiments that the electromagnetic radiation energy of a substance will vary when stress acts on the substance. This moment, the electromagnetic radiation energy (observation value) received by the remote sensor is triggered not only by the substance temperature and also by the stress. Separating quantitatively these two kinds of electromagnetic radiation energy and then inversing the actual temperature state and stress state of a medium is a matter with practical significance in earthquake prediction and stability monitoring for the large-scale geotechnical engineering. In this paper the principle and the mathematical method for inversing stress by using multiband remote sensing data are discussed in detail. A calculation example is listed.  相似文献   
80.
This study provides a detailed magnetostratigraphic record of subsidence in the Linxia Basin, documenting a 27 Myr long sedimentary record from the northeastern edge of the Tibetan Plateau. Deposition in the Linxia Basin began at 29 Ma and continued nearly uninterruptedly until 1.7 Ma. Increasing rates of subsidence between 29 and 6 Ma in the Linxia Basin suggest deposition in the foredeep portion of a flexural basin and constrain the timing of shortening in the northeastern margin of the plateau to Late Oligocene–Late Miocene time. By Late Miocene–Early Pliocene time, a decrease in subsidence rates in the Linxia Basin associated with thrust faulting and a 10° clockwise rotation in the basin indicates that the deformation front of the Tibetan plateau had propagated into the currently deforming region northeast of the plateau.  相似文献   
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