基于广义Kопытов模型及乙型水驱曲线的综合预测法

将广义Kопытов预测模型和乙型水驱曲线方法有机的结合起来，得到了油田开发中后期——递减时期的一种预测水驱开发油田的含水率、产油量、产水量及其相应的累积产量随开发时间变化的方法，此方法克服了在水驱油田预测开发指标中二者所存在的局限性。     

四川盆地碳酸盐岩油气勘探实践与认识

四川盆地烃源十分丰富。但油气演化程度高,大多已进入高成熟和过成熟阶段,至今只在侏罗系发现有油藏,三叠系及其更老地层皆为气藏。储层主要为碳酸盐岩,其特点是低孔低渗,平均孔隙度仅1.7%,平均渗透率小于1×10~(-3)μm~2,但其中的“孔洞发育层段”平均孔隙度可达3%～6%。根据四十年的勘探经验,加强预探并争取新发现是四川盆地油气勘探发展的关键。预探中,按构造带规划大中型气田勘探目标,将成藏条件相似、地域上相邻的局部圈闭群作为一个整体勘探对象,实行稀井广探,少井高效。“八五”以来,在高陡构造带勘探技术、储层横向预探技术等方面有长足的进步,勘探成效不断提高,实现了资源序列的良性循环。     

Economic valuation of policies for managing acidity in remote mountain lakes: Examining validity through scope sensitivity testing

No Abstract. .The following two amendments concern the above mentioned article that appeared electronically Online First on June13, 2005 (this issue, pp. 274–291).1. the first name of the author Cooper is Philip (and not Phillip).2. the correct grant reference number is EVK1-CT-1999-00032 (instead of: EVK1-CT-2002-00121).     

苏鲁超高压变质带岗上石榴石橄榄岩岩体：中国大陆科学钻探卫星孔（CCSD-PP3钻孔）初步研究

大陆科学钻探在江苏岗上超镁铁岩体上打了一个卫星孔(CCSD-PP3),孔深705m,穿透428m厚超镁铁岩体,其下主要为不同类型片麻岩及少量榴辉岩。该岩体产在苏鲁超高压变质带中,面积1370×700m,上覆约10m厚第四纪盖层。岩心柱可以粗分为4段,370m上部超镁铁岩,50m片麻岩夹榴辉岩,60m下部超镁铁岩,225m片麻岩类。榴辉岩夹在片麻岩中,片麻岩有正、副之分。榴辉岩石榴石中发现柯石英假象,表明岩石经历超高压变质作用。超镁铁岩主要岩性为纯橄岩和含石榴石纯橄岩,含石榴石纯橄岩出现3层,总厚度仅90m,与不舍石榴石的纯橄岩无截然界线。岩相学研究观测到石榴石中保留橄榄石、单斜辉石和尖晶石等超高压变质之前的矿物组合,以及退变质矿物替代石榴石的现象。岩石化学成分总体变化小,SiO242.17-44.79,平均43.78;MgO46.35-48.98,平均47.42,Mg#值(=Mg/(Mg Fe)×100)为91.89-92.75,平均92.4,属于高Mg型;Al2O3和CaO丰度低,分别为0.66-0.27,平均0.43,和0,01-0.35,平均0.13;REE总量较原始地幔亏损,但LREE相对HREE富集。结合矿物组合特征,说明这套岩石属亏损型,但可能经历了流体热液的改造;纯橄岩和含石榴石纯橄岩成分的一致型,说明后者是前者经变质改造形成。SHRIMPU-Pb定年测得含石榴石纯榄岩中锆石存在两组年龄,超高压变质阶段新形成的锆石时代为240±2.7Ma,核部残留岩浆锆石给出726±56Mao前者与区域上超高压变质年龄十分吻合,后者与大别-苏鲁区域上新元古代大规模花岗质岩浆侵位时代。岗上超镁铁岩体可能记录了早期侵位到地壳,在陆陆俯冲碰撞阶段被俯冲岩片带入到柯石英形成深度,以及随岩片折返到地表的整个历史。     

Coronal environment of quiescent prominences

With thespectro-coronagraph and themultichannel subtractive double pass spectrograph (MSDP) at the Pic du Midi Observatory two quiescent prominences were observed simultaneously. From the spectro-coronagraph observations 2D maps of Hei 10830 , Fexiii 10798 and 10747 line intensities were obtained. In addition, we obtained 2D maps of the ratioR of the two iron lines. This ratio is used as a diagnostic for determining the density of the hot coronal plasma surrounding prominences. We found that the electron density is higher at the location of the prominences than in the corona, whereas small regions (40) of lower electron density are unevenly distributed around the prominences indicating that the surrounding corona is highly inhomogeneous. The density of the cavity is reduced by a factor 1.5 compared to the density of the prominence environment (5 × 10⁸ cm^–3). We discuss the existence of cavities around these prominences according to the orientation of their axes relative to the line of sight and according to the velocity field inside the prominences. Constraints on models for prominence formation are derived.     

Multi-wavelength observations of the onset phase of a coronal mass ejection

The structure and dynamics of the initial phases of a coronal mass ejection (CME) seen in soft X-ray, extreme ultraviolet and optical emission are described. The event occurred on the SW limb of the Sun in active region AR 8026 on 9 April 1997. Just prior to the CME there was a class C1.5 flare. Images taken with the Extreme Ultraviolet Imaging Telescope (EIT) reveal the emergence of a candle-flame shaped extreme ultraviolet (EUV) cavity at the time of the flare. Yohkoh images, taken about 15 min later, show that this cavity is filled with hot X-ray emitting gas. It is most likely that this is the site of the flare. Almost simultaneous to the flare, an H surge or small filament eruption occurs about 50 arc sec northwards along the limb from the EUV cavity. At both the site of the core of the hot, EUV cavity and the filament ejection are X-ray jets. These jets seem to be connected by hot loops near their bases. Both jets disappear within a few minutes of one another.Clear evidence of the CME first appeared in the Large Angle Spectrometric Coronagraph (LASCO) and EIT images 40 min after the flare and onset of the filament ejection. It seems to come from a region between the two X-ray jets. This leads to the speculation that magnetic field reconnection near one footpoint of a loop system triggers reconnection near its other footpoint. The loop system is destabilized and ultimately gives rise to the CME. This possibility is supported by magnetic field and H images taken when the active region was at disk center which show that the active region had a double bipole structure with dark H filaments between the bipoles.     

Climate variability and trends in downscaled high-resolution simulations and projections over Metropolitan France

In order to fulfill the society demand for climate information at the spatial scale allowing impact studies, long-term high-resolution climate simulations are produced, over an area covering metropolitan France. One of the major goals of this article is to investigate whether such simulations appropriately simulate the spatial and temporal variability of the current climate, using two simulation chains. These start from the global IPSL-CM4 climate model, using two regional models (LMDz and MM5) at moderate resolution (15–20 km), followed with a statistical downscaling method in order to reach a target resolution of 8 km. The statistical downscaling technique includes a non-parametric method that corrects the distribution by using high-resolution analyses over France. First the uncorrected simulations are evaluated against a set of high-resolution analyses, with a focus on temperature and precipitation. Uncorrected downscaled temperatures suffer from a cold bias that is present in the global model as well. Precipitations biases have a season- and model-dependent behavior. Dynamical models overestimate rainfall but with different patterns and amplitude, but both have underestimations in the South-Eastern area (Cevennes mountains) in winter. A variance decomposition shows that uncorrected simulations fairly well capture observed variances from inter-annual to high-frequency intra-seasonal time scales. After correction, distributions match with analyses by construction, but it is shown that spatial coherence, persistence properties of warm, cold and dry episodes also match to a certain extent. Another aim of the article is to describe the changes for future climate obtained using these simulations under Scenario A1B. Results are presented on the changes between current and mid-term future (2021–2050) averages and variability over France. Interestingly, even though the same global climate model is used at the boundaries, regional climate change responses from the two models significantly differ.     

1∶25万那曲县幅地质调查成果与进展

地层方面,将测区地层划分为冈底斯腾冲地层区和班公错 怒江结合带,班公湖 怒江结合带中又划分出聂荣微地块和觉翁 余拉山 下秋卡混杂带两个小区;按变质岩调查方法解体了聂荣地块;对原大面积分布的拉贡塘组进行了有效的解体;新建立嘎加组;恢复了郭曲群;将木嘎岗日岩群解体出3个岩组。岩石方面,在测区南部新发现了一套晚二叠世—早三叠世蛇绿岩。构造方面,构造单元表现为各组 下秋卡结合带和桑雄那曲 麦地卡板片的构造格局;新发现达仁乡夺列蛇绿岩体。     

伸展地区铲式正断层作用及其大地测量观测

铲式正断层作用是伸展构造区最主要的构造运动形式。本文根据铲式正断层作用的几何学、运动学特征,结合华北平原伸展区大地测量观测成果,探讨伸展区构造形变铲式正断层现今活动的地表形变效应及其动态特征。