池州地区冬半年固态降水及其环流背景统计特征

基于2003－2018年池州冬半年观测资料,采用T-mode主成分客观分析法（TPCA）等方法进行固态降水与环流背景的统计分析。结果表明：池州172个固态降水日中,固态降水的主要月份占比分别是1月的44.8%、2月的27.9%和12月的16.3%;其中雨雪转换、纯雪和冻雨3类占比分别为55.2%、41.3%和3.5%。环流形势可划分为一槽一脊型（Ⅰ型）,纬向波动型（Ⅱ型）和两槽一脊型（Ⅲ型）,Ⅰ型占比最多,Ⅱ型次之,Ⅲ型较少。Ⅰ～Ⅲ型分别代表北方冷空气从中路、西路和东路南下,池州固态降水过程主要受中路冷空气影响。Ⅰ型气温最低,出现固态降水概率最高,是其它形势3倍以上;Ⅱ型气温最高,出现固态降水概率最低。除Ⅲ型外,纯雪过程中低层温度均较雨雪转换过程低2.0 ℃左右;雨雪转换过程中925 hPa温度与850 hPa基本相同,一般在-4.0～-5.0 ℃之间,而纯雪过程则较850 hPa偏高1.0 ℃左右;雨雪转换过程1000 hPa温度基本在0 ℃附近,纯雪则在0 ℃以下。925 hPa盛行东北风,850 hPa存在气旋性环流,配合700 hPa上12.0 m/s左右急流、水汽通量及水汽通量散度大值中心,有利于池州固态降水的产生。它一般属于大尺度降水,层结稳定,锋区位于700 hPa以下,低层有冷平流,切变线一般位于850～800 hPa之间。     

亚暴事件中磁尾多重等离子体团的数值研究（Ⅰ）

GEOTAIL卫星于1994年1月15日亚暴期间,在深磁尾（x＝96RE）观测到多重等离子体团及与之相对应的高能离子爆,作者以宁静磁尾平衡位形为初态,考虑介质的可压缩性,数值研究亚暴期间磁尾动力学过程．计算结果展现了等离子体团间歇性形成及其运动发展过程．体现了强亚暴事件中储存于碰尾的能量,通过多重等离子体团的排放而逐渐释放的进程．数值结果还表明：持续施加于边界上的晨昏电场及由此引发的驱动重联是导致等离子体团准周期形成的主要因素．此外,作者还考察尾瓣内任一点磁场强度及其分量随时间的演化,它与行进压缩区（TCRs）的观测特征基本相符．     

Distribution characteristics of delta reservoirs reshaped by bottom currents: A case study from the second member of the Yinggehai Formation in the DF1-1 gas field,Yinggehai Basin,South China Sea

The Dongfang1-1 gas field (DF1-1) in the Yinggehai Basin is currently the largest offshore self-developed gas field in China and is rich in oil and gas resources. The second member of the Pliocene Yinggehai Formation (YGHF) is the main gas-producing formation and is composed of various sedimentary types; however, a clear understanding of the sedimentary types and development patterns is lacking. Here, typical lithofacies, logging facies and seismic facies types and characteristics of the YGHF are identified based on high-precision 3D seismic data combined with drilling, logging, analysis and testing data. Based on 3D seismic interpretation and attribute analysis, the origin of high-amplitude reflections is clarified, and the main types and evolution characteristics of sedimentary facies are identified. Taking gas formation upper II (IIU) as an example, the plane distribution of the delta front and bottom current channel is determined; finally, a comprehensive sedimentary model of the YGHF second member is established. This second member is a shallowly buried “bright spot” gas reservoir with weak compaction. The velocity of sandstone is slightly lower than that of mudstone, and the reflection has medium amplitude when there is no gas. The velocity of sandstone decreases considerably after gas accumulation, resulting in an increase in the wave impedance difference and high-amplitude (bright spot) reflection between sandstone and mudstone; the range of high amplitudes is consistent with that of gas-bearing traps. The distribution of gas reservoirs is obviously controlled by dome-shaped diapir structural traps, and diapir faults are channels through which natural gas from underlying Miocene source rocks can enter traps. The study area is a delta front deposit developed on a shallow sea shelf. The lithologies of the reservoir are mainly composed of very fine sand and coarse silt, and a variety of sedimentary structural types reflect a shallow sea delta environment; upward thickening funnel type, strong toothed bell type and toothed funnel type logging facies are developed. In total, 4 stages of delta front sand bodies (corresponding to progradational reflection seismic facies) derived from the Red River and Blue River in Vietnam have developed in the second member of the YGHF; these sand bodies are dated to 1.5 Ma and correspond to four gas formations. During sedimentation, many bottom current channels (corresponding to channel fill seismic facies) formed, which interacted with the superposed progradational reflections. When the provenance supply was strong in the northwest, the area was dominated by a large set of delta front deposits. In the period of relative sea level rise, surface bottom currents parallel to the coastline were dominant, and undercutting erosion was obvious, forming multistage superimposed erosion troughs. Three large bottom current channels that developed in the late sedimentary period of gas formation IIU are the most typical.     

末次冰期以来中国自然环境变迁及其与全球变化的关系

末次冰期我国西部的冰川长度比现代冰川长2—5倍,雪线低300—1080m;东部多年冻土区南界在33°20′—33°40′N,青藏高原多年冻土区东北部的下界在海拔2200—2600m 处;黄、东海海平面下降130—155m;经向环流加强,北方冷空气增强。末次冰期以后冰川阶段性退缩,多年冻土区阶段性缩小,海平面间歇性上升;8000—6000aB.P.为高温期,出现2—5m 高海面,5600—5000aB.P.气温短暂下降,海平面突然回落,冰川有所前进;3000aB.P.的新冰期和15—19世纪的小冰期,气候、冰川和海平面都有显著变化。哺乳动物的绝灭和迁徙是自然和人为双重影响的结果。这些变化都是全球变化的表现。     

晨昏起伏电场对中性片离子的随机加热

本文从哈密顿原理出发,讨论磁尾中性片中粒子受晨昏起伏电场的影响问题,并把它归结于讨论标准映射的性质.中性片本身是非线性系统,外加起伏场会导致其进入混沌状态.本文计算了进入该状态的临界电场E_c以及不同E下的粒子轨迹.计算表明,观测到的晨昏电场可以使离子进入混沌状态,但远小于电子的临界场值.这样离子运动是随机的,电子运动是规则的.仅对离子的随机加热可能是导致中性片中离子温度高于电子温度的原因.     

楚雄盆地下侏罗统磨拉石楔沉积与含油性研究

楚雄盆地为一中生代周缘型走滑前陆盆地。通过对下侏罗统冯家河组沉积特征的详细研究与对比,作者认为早侏罗世是楚雄前陆盆地强烈坳陷与沉降的主要发展时期,从早期到晚期经历了一个突然变深又变浅的典型前陆盆地充填过程。在前陆冲断块体的不断逆冲和加载条件下,楚雄盆地西部早侏罗世沉积物的来源主要为哀牢山造山带隆起,其沉积环境以滨、浅湖或湖泊三角洲为主。位于盆地东北部的永仁中和、大姚龙街等地区的早侏罗世沉积物则来源于元谋古隆起,沉积特征亦显示其为滨、浅湖或湖泊三角洲相。位于盆地中部的楚雄会基关地区(楚参一井),下侏罗统沉积厚度急剧增加,测井曲线、录井资料以及岩心薄片鉴定、粒度分析均显示其沉积环境为深湖央浊积砂体。在新平叠社莫一带也发现有深湖相泥灰岩或灰泥岩沉积。由此表明,早侏罗世楚雄前陆盆地的沉降与沉积中心已经从晚三叠世的古哀牢山前缘向NE迁移至楚雄会基关以及新平叠社莫一带,盆地内的沉积物呈明显的前陆楔形体充填。大姚龙街地区冯家河组第三段中首先发现的沥青砂岩进一步增强了楚雄盆地产油气的可能性。根据产状,沥青砂岩分为缝隙型和粒间孔型两类,它们同产于逆韵律结构发育的湖泊三角洲相沉积层序。因此,对该区下侏罗统缝隙型圈闭以及岩性圈闭构造应予以足够的重视。     

楚雄复式盆地演化及形成的动力学机制

楚雄盆地处于中国云南省中部,位于扬子板块西南缘,南西界以红河断裂为界与哀牢山造山带相连,北西界为程海断裂,东边为绿汁江断裂。盆地基底包括结晶基底和褶皱基底双重结构。盆地内发育了中三叠世以后的沉积盖层,西部中三叠世和晚三叠世早、中期为海相沉积,晚期为海陆交互相和陆相沉积;盆地东部为陆相沉积。侏罗-白垩纪整个盆地为巨厚的陆相沉积。楚雄盆地的构造格架分为4个带:(1)哀牢山造山带;(2)褶皱逆冲带;(3)中部沉降带;(4)东部隆起带。盆地形成与演化分为六个阶段:(1)被动大陆边缘沉降阶段;(2)拉张热隆起边缘——裂谷盆地阶段;(3)沟一弧一盆系阶段;(4)残洋一周缘前陆盆地阶段;(5)走滑一拉张盆地阶段;(6)走滑-挤压-改造阶段。楚雄盆地的形成与演化体现了盆地动力学性质转化和复合,在多种动力系统作用下或经过多旋回构造阶段产生了复式盆地。     

Dynamic response of road pavement resting on a layered poroelastic half‐space to a moving traffic load

This paper is dedicated to study the dynamic response of a thin‐plate resting on a layered poroelastic half‐space under a moving traffic load. Based on the dynamic poroelastic theory of Biot, the general solutions of the homogeneous poroelastic foundation are obtained by Fourier translation. By using the transmission and reflection matrices method in the frequency domain, the equivalent stiffness of the layered poroelastic half‐space is presented. Kirchhoff's hypotheses are applied to obtain the vertical displacement of the thin plate. By using the inverse Fourier transform, the time domain solution is obtained. As an example of three layers, the influences of the load velocity, the material properties of poroelastic layers, and the flexural rigidity of the plate on the response of the pavement system are examined. Analyses show that a soft intermediate layer results in the significant increase of vertical displacement of road pavement. Comparison with the existing work validates the present model. Copyright © 2013 John Wiley & Sons, Ltd.     

13．7m抛物面天线增益测量和太阳射电流量密度定标

以新月时月亮的射电辐射为温度基准和准口面温度定标的方法，在２２ＧＨｚ频率上于１９９３年７月～３月测量了１３．７ｍ射电望远镜抛物面天线的增益。根据测量的增益值（６７．１０─±０．０７ｄｂ）定标了太阳射电流量，流量测量的系统差为±５．８％，偶然差为±２．７％，测量的宁静太阳亮温度（非源区）为１０１００±３００Ｋ。除此之外，还推导和计算了不同源模型下的天线方向图改正因子Ｋｓ，并计算了太阳射电源的流量密度。     

相速、群速和能量传播速度

本文论述群速和能量传播速度的基本概念,并对相速、群速及能量传播速度的联系及区别作了讨论。