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991.
J. Gani P. Todorovic 《Stochastic Environmental Research and Risk Assessment (SERRA)》1987,1(3):209-216
A simple two-dimensional random walk model is developed for the motion of a particle in a fluid flow. Some earlier results for the persistent injection of particles into the flow are extended, and the distribution of the maximum number of particles in suspension over the period (0,t) is derived. 相似文献
992.
993.
西藏阿里西部地区中、酸性侵入岩广泛分布在冈底斯、北喜马拉雅、高喜马拉雅三个构造带中。钾-氩同位素年龄为189—2.2Ma,可以分为燕山早期、中期、晚期,喜山早期、中期五个侵入期。岩石化学、稀土元素和锶同位素的研究表明,形成本区石英闪长岩和花岗闪长岩的岩浆,来源于下地壳;形成花岗岩的岩浆,来源于上地壳. 相似文献
994.
叶树林 《华东地质学院学报》1987,(1)
本文在大量实验和实践工作的基础上,对钋法找矿探测深度、钋室内分析流程(简称流程)的一些影响因素及土样化学成分对流程的影响等问题进行讨论。同时,对钋法找矿中采用归一化流程的可行性、必要性进行了论述。因而本文对钋法找矿工作的开展有一定的实际参考价值。 相似文献
995.
中国东北地区新生代火山岩的年代学研究 总被引:36,自引:19,他引:36
用常规K-Ar、~(40)Ar-~(39)Ar、~(14)C等方法系统测定了东北地区新生代火山岩的年龄,获得近百个有效年龄数据。其精度和准确度都很高,与地质背景相当吻合。对于玄武岩中超镁铁质岩色体也进行了年龄测定尝试、发现包体中含继承氩,并可能存在~(36)Ar过剩。在阶段加热过程中,样品中氩的释放有两个高峰,一个在低温阶段(450—620℃),另一个在高温阶段(>1000℃),约50%的放射成因~(40)Ar在低温阶段释放。 相似文献
996.
997.
The Mangalur greenstone belt of Dharwar Craton, South India, is an Archaean schist belt dominated by metavolcanic rocks. The
gold mineralization occurs within the metavolcanics and the fabric, mineralogy and geochemistry of these host rocks indicate
that they were tholeiitic basalts regionally metamorphosed under medium to low-grade greenschist facies. The basic metavolcanic
rocks occur as tholeiitic metabasalts and amphibolites. The rocks have undergone some fractionation and appear to be derived
from melts generated by 10 to 25% melting of the mantle at depths 30 to 35 km around temperature 1200°C and pressure 12 kb.
The source of gold is mainly in the basalts and not in the surrounding granites. 相似文献
998.
滇东-黔西地区晚二叠世煤岩及煤层气储层物性分析 总被引:3,自引:0,他引:3
本文以丰富的地质资料对滇东-黔西地区晚二叠世煤岩分布的割理(裂隙),吸附、孔隙溶积、镜质组含量、含气性、灰分产率等进行了较为系统的研究,初步建立了煤炭与煤层气储层物性的关系,提出了镜质组含量的煤炭类型有较好的煤层气储集物性条件。 相似文献
999.
Low frequency electrostatic waves are studied in magnetized plasmas with an electron temperature which varies with position in a direction perpendicular to the magnetic field. For wave frequencies below the ion cyclotron frequency, the waves need not follow any definite dispersion relation. Instead a band of phase velocities is allowed, with a range of variation depending on the maximum and minimum values of the electron temperature. Simple model equations are obtained for the general case which can be solved to give the spatial variation of a harmonically time varying potential. A simple analytical model for the phenomenon is presented and the results are supported by numerical simulations carried out in a 2.5-dimensional particle-in-cell numerical simulation. We find that when the electron temperature is striated along B0 and low frequency waves (ci) are excited in this environment, then the intensity of these low frequency waves will be striated in a manner following the electron temperature striations. High frequency ion acoustic waves (ci) will on the other hand have a spatially more uniform intensity distribution. 相似文献
1000.
Hydrodynamical Modeling Of Oceanic Vortices 总被引:1,自引:0,他引:1
Xavier Carton 《Surveys in Geophysics》2001,22(3):179-263
Mesoscale coherent vortices are numerous in the ocean.Though they possess various structures in temperature and salinity,they are all long-lived, fairly intense and mostly circular. Thephysical variable which best describes the rotation and the density anomaly associated with coherent vortices is potential vorticity. It is diagnostically related to velocity and pressure, when the vortex is stationary. Stationary vortices can be monopolar (circular or elliptical) or multipolar; their stability analysis shows thattransitions between the various stationary shapes are possible when they become unstable. But stable vortices can also undergo unsteady evolutions when perturbed by environmental effects, likelarge-scale shear or strain fields, -effect or topography. Changes in vortex shapes can also result from vortex interactions. such as the pairing, merger or vertical alignment of two vortices, which depend on their relative polarities and depths. Such interactions transfer energy and enstrophy between scales, and are essential in two-dimensional and in geostrophic turbulence. Finally, in relation with the observations, we describe a few mechanisms of vortex generation. 相似文献