辽河小洼油田东营组沉积环境条件的研究

陆相盆地沉积作用主要受构造作用及古气候的控制，所以从区域构造背景出发，结合地层、古生物、沉积、地球化学等方面资料，对小洼油田东营组的沉积环境条件进行综合分析。确定了沉积物源来自北东方向的中央凸起，古气候属于半干旱—半潮湿的温带气候条件，水介质是弱还原性的淡水滨浅湖泊沉积环境。此时中央凸起上丰富的风化剥蚀产物经过河流的搬运和分异作用，进入湖盆中形成三角洲沉积体     

辽西中生代火山岩岩浆成因——稀土元素配分及同位素定量模式

本文通过对辽西及邻区中生代盆地火山岩稀土元素配分特征的研究及模拟运算，探讨了其岩浆成因及过程。结果显示南北岩区岩浆成因不同，南岩区岩源为MORB地幔和长期富集型幔熔融混合而成，北岩区为MORB和近期亏损型地幔熔融混合而成。     

我国特殊岩土研究

本文分析，总结了我国特殊岩土理论与应用研究方面的新进展，内容涉及湿陷性黄土，软土膨胀岩土，红土，软岩和特殊土的结构性，指出需要进一步研究的问题，最后对特殊土的研究方法做了阐述。     

黑龙江省砂金的成色特征

对黑龙江省８４个砂金样品的成色进行测定了并与７个岩金样品对比，结果表明，砂金成色变化较大，与原生岩金来源有明显继承性关系，由于受后生风化作用影响，砂金普遍具有金壳结构。砂金成色与其粒度及在河谷中产出位置呈规律性变化，由成色计算出来的溶蚀系数，可作为指导寻找原生金矿的依据之一。     

脉金矿床控矿条件及源区性质刍议

目前对脉金矿床，特别是大型金矿床的形成研究已取得重要进展，它在时间和空间上具有明显的一致性表明：大型脉金矿床的形成与特定的地质背景有密切关系，矿源具有深源性质，而与探矿岩系金的丰度值基本无关。     

Formation Environment of the High-Pressure Metamorphic Rocks, Western Tianshan, Xinjiang, China

1.IntroductionFromexperimefltalphaseequilibrium,stableisotOPe,andthermo-barometricstudies,ProgradebineschistdineralparageneseshavebeenproducedexclusivelyatrelativelyhighPadratios(DeRoever,1956;Miyashiro,1961;DobretsovandSobolev,1984;Emst,1973,1988;Maruyamaetal.,1996).InthelastthreedeCades,withtheadvanceofplatetectonics,manygeologistssuggestedthatblueschists,representinghigh-Pressurelow-tCmperamre~rphism,areformedbysubductionofoceanicplate(Emst,1973).Blueschistshavealsobeenregardedasoneof…     

冀西北东坪金矿床成矿流体的来源研究

冀西北东坪金矿床成矿流体的来源研究＊莫测辉王秀璋程景平梁华英（华南农业大学资源环境学院，广州５１０６４２）（中国科学院广州地球化学研究所，广州５１０６４０）关键词金矿床成矿流体来源岩浆热液大气降水热液侵入岩体中的金矿床乃至岩体接触带或附近地层中的金矿...     

三江地区高吉碱性岩体的岩石化学特征

三江地区的碱性岩有其独特的地质、岩石学与岩石化学特征；这些特征所记录的信息，不仅提供了高吉碱性岩区别于邻区及其它地方同类碱性岩的证据，而且也给出了识别碱性岩的标志与判定其所处的板块构造位置。     

浙江省安吉县山区竹类资源综合利用

安吉县竹类资源优势突出 ,使其综合利用已初具规模 .竹业工业已成为新兴工业门类 .竹业经济已是地方经济的一个台柱子 .但竹业结构不合理 ,竹制品雷同性大 ,增值率低 ,资源供需矛盾突出等日益明显 .对今后竹类资源综合利用和持续发展 ,提出了主要思路     

The Zihuatanejo, Mexico, earthquake of 1994 December 10 (M= 6.6): source characteristics and tectonic implications

An analysis of the Zihuatanejo, Mexico, earthquake of 1994 December 10 ( M = 6.6), based on teleseismic and near-source data, shows that it was a normal-faulting, intermediate-depth ( H = 50 ± 5 km) event. It was located about 30 km inland, within the subducted Cocos plate. The preferred fault plane has an azimuth of 130°, a dip of 79° and a rake of −86°. The rupture consisted of two subevents which were separated in time by about 2 s, with the second subevent occurring downdip of the first. The measured stress drop was relatively high, requiring a Δσ of about a kilobar to explain the high-frequency level of the near-source spectra. A rough estimate of the thickness of the seismogenic part of the oceanic lithosphere below Zihuatanejo, based on the depth and the rupture extent of this event, is 40 km.
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event.