辉石巨晶中的硫化物及其成因

我国一些地区玄武岩辉石巨晶中的硫化物球泡(0.02-0.05mm)呈点阵式、散布式、定向带状或微裂隙羽状分布。硫化矿物组合是磁黄铁矿-镍黄铁矿-黄铜矿,其中以磁黄铁矿为主(～90％)。根据硫化物的规则排布以及高温矿物组合推测点阵式、散布式硫化物形成于地幔。是由溶解了～1％S的硅酸盐熔体在减压上升过程中析出过饱和的硫所致。     

华南两个成岩成矿系列花岗岩中黑云母的差热分析

本文对采自华南两个成岩成矿系列花岗岩中的黑云母进行了DTA特征和其他热性质的比较。发现可根据黑云母的OH脱失峰温度、熔化吸热峰的形状、熔化热及熔化后产物的形态来区分不同成因的花岗岩。文中还探讨了造成黑云母热性质差异的原因。     

横断山不同成因类型花岗岩类岩石中黑云母的标型特征

本文研究了横断山区不同成因类型花岗岩类岩石中黑云母的化学成分、微量元素、结构和物理性质等。结合花岗岩类岩石的成因类型,将黑云母分为三个亚种:富镁黑云母(MF=1.3—1.5)、镁黑云母(MF=1—1.3)和富铁黑云母(MF=0.5-1)。     

黄钇钽矿形成条件的实验研究

本文实验表明,黄钇钽矿需要在温度≥500℃,溶液pH≈4.0-7.5,压力500—1500bar的范围内形成,与褐钇铌矿相比,其形成条件的范围要窄得多。 不同的稀土元素在形成黄钇钽矿时的成矿温度亦不同。钇族稀土成矿温度相对较低且相互接近,铈族稀土的成矿温度比钇族稀土高得多,并随原子序数减小而迅速增高,以致La、Ce、Pr、Nd在一般的地质条件下难以形成这种结构的矿物,这就是至今在自然界发现的黄钇钽矿均为钇族稀土占优势的原因之一。实验还表明,大量F、P等组分的存在,对黄钇钽矿的形成是不利的。     

研究超镁铁岩中八面体假象蛇纹石和绿泥石的地质意义

继1981年首次报导八面体假象蛇纹石之后,在同一超镁铁岩中又发现了一些八面体假象含铬绿泥石,后者是交代前者的产物。通过研究我们认为:1)八面体假象绿泥石中的Al、Cr等元素来自铬铁矿石;2)和八面体假象蛇纹石一样,八面体假象绿泥石的最初原生矿物也应为γ一橄榄石,后者的形成压力为140×10~8Pa(140Kb),相当于500公里的深度;3)包有八面体假象蛇纹石和绿泥石的铬铁矿可能是一种直接来自深部地慢的铬铁矿类型;4)藏北岩带的两处(安多和阿里地区)超镁铁岩中出现八面体假象矿物说明藏北超镁铁岩带(或岩带的几处超镁铁岩)形成的构造环境可能深于藏南超镁铁岩带。     

Seismotectonic scheme of Central and Eastern Europe

Summary The distribution of earthquake foci in the crust and the upper mantle indicates the position of mobile zones. Comparing epicentral maps of Central and Eastern Europe, known tectonic lines, results of deep seismic sounding and gravimetric survey enables a scheme of potential seismogenic zones, which correspond to active fault zones separating plates and blocks in the area, to be compiled. The level of earthquake activity varies along the investigated boundaries and can be considered as a measure of the intensity of the present geodynamic processes.Paper presented at the joint symposium AlO of the XVIIth General Assembly of the European Seismological Commission and of the 7th Annual Meeting of the European Geophysical Society, Budapest (Hungary), Aug. 21. – 29., 1980.     

Analysis of beam nulling of a sharpe gravity meter

Summary The routine nulling procedure is modified on the basis of the theoretical decay of transient motion of the gravity meter beam and the time needed for its stabilizing.     

On the spiral structure of atmospheric vortices

a au au a ¶rt;am m ¶rt;uauu n¶rt;nu mau nua am u nu uu, m n amu n nua n uau mua mu.     

A simple model of a building cumulus cloud

Summary A model of a building cumulus structure is described. The one-stage model published in[1] was used to describe ascent of two cloudy parcels that a cloud is supposed to be formed of. The other ascent is assumed to take place after the first cloud element sinks back as a result of evaporative cooling. The numerical results and their evaluation are given for various rates of mixing at the cloud top level of the first cloud volume.     

Time pattern of large earthquake sequences in Europe in 1976–1979

Summary The time development of three large sequences, Friuli 1976, Thessaloniki 1978 and Monte Negro-Albania 1979, was investigated by analysing the characteristics of the time distribution of magnitudes of the events, M(t), of average magnitudes, (t), and of the number of events, n(t), as well as the strain release curves and the magnitude-frequency relations, N(M). The existence of time gaps and of an anomalous decay of the numbers of shocks before major events, as well as the oscillation of ( const b^–1) may be considered as precursory phenomena. The clustering of events has been tested by the Poisson and negative binomial laws.Communication presented at the XVIIth General Assembly of the European Seismological Commission in Budapest, 21–29 August, 1980 under the title Properties of Seismic Regime and Recent Earthquake Sequences in Europe.