光谱样品中银的测定

样品经酸溶后,加碘化钾,银以AgI方式存在,有机试剂萃取分离,用原子吸收分光光度计测定有机相中银的含量,测定范围(1~1 000)×10-9。     

鄂尔多斯盆地陕北地区长7砂岩储层成岩相特征研究

在大量样品测试数据与野外地质调查综合分析的基础上, 对长7储层岩石学特征、物性、孔隙结构、成岩作用、成岩阶段和成岩相等进行了研究。结果表明: 研究区长7储层处于中成岩A~B期。压实作用及碳酸盐、粘土(高岭石、伊利石、伊蒙混层)矿物胶结和硅质胶结作用是造成储层原生孔隙丧失的主要原因; 绿泥石胶结抑制孔隙充填, 长石溶蚀作用使孔隙间的连通性得到改善, 储层物性得到提高。根据成岩作用类型、强度及其对储层物性的影响划分出6种成岩相, 其中压实相、碳酸盐胶结相、粘土矿物胶结相、石英加大相、浊沸石充填相不利于储层的发育, 而长石溶蚀相、绿泥石膜胶结相对储层物性改善起了重要作用。     

西南三江地区造山演化过程及成矿时空分布

三江地区单凭“一次造山”是难以圆满解释的。本文试以“多次造山”多期成矿”的思路作出合理说明。晚古生代－中生代早期多岛海造山阶段,羌塘弧、江达弧和临沧弧应为前锋弧,其后由一系列弧后盆地和岛弧或残余弧（或微大陆）组成。中生代中－晚期为陆内俯冲造山阶段,推测金沙江带、哀牢山带和龙门山－锦屏山带为俯冲主边界,从而形成本区燕山期重熔型花岗岩带,控制相应矿产的分布特征。新生代陆内转换造山阶段,造成特征的构造－岩浆－成矿带,具有生成大型或超大型矿床的潜力。     

近55年广西融水县降水气候特征分析

利用融水县气象站1959-2013年的降水资料,采用数理统计和线性倾向估计分析方法,分析了融水县降水分布特征及其变化规律。结果表明：融水县降水分配不均,主要集中在4-8月,6月最多,5月次之;年暴雨日数6.9d,暴雨持续时间多为1d,最长4d;近55年来融水县年降水量和汛期（4-9月）降水量均呈减少趋势,每10年分别减少16mm和6mm,而主汛期（5-8月）的降水量却呈增多趋势,每10年增加13mm,这预示着融水县未来降水可能更趋于集中在主汛期（5-8月）,发生洪涝灾害的几率可能增多。此外,一日最大降水量呈增多趋势,预示未来降雨强度可能增大;春、秋季的降水量呈减少趋势,提示未来发生春旱、秋旱的几率可能增多。     

运城市2010年4月13日强霜冻过程分析

利用常规天气资料和数值预报产品,应用天气分析和诊断分析方法,对2010年4月13日运城市出现的近40年最严重的强霜冻天气过程进行分析,并与历史个例进行比较,结果表明,此次过程是在前期升温明显的基础上,有强冷空气在西伯利亚及贝加尔湖堆积并向南侵袭造成的;此次过程亚洲中高纬环流表现为“一脊一槽”型,动力机制为横槽转竖促使冷空气向南爆发;冷空气爆发后,本地上空由强盛的冷平流控制,地面冷高压进入关键区并达到寒潮强度。由于每次强降温发生的环流背景、影响系统及冷空气的强度、发展、移动路径不同,所以造成的降温幅度和影响也不同。在此基础上,总结出强霜冻预报的着眼点。     

联合像元-深度-对象特征的遥感图像城市变化检测

特征空间的构建和优化对遥感图像识别能力的提高具有重要作用。针对面向对象方法对波段光谱信息利用不足,以及像元识别法无法充分利用图像空间几何等信息的问题,本文建立了新颖的联合像素级和对象级特征的航摄遥感图像城市变化检测方法。首先,充分利用像素级和对象级特征的优势,建立考虑光谱、指数、纹理、几何、表面高度及神经网络深度特征的特征空间;然后,引入LightGBM(light gradient boosting machine)算法对大量特征进行选择研究;最后,采用随机森林识别器对宜兴市2012年和2015年两期遥感图像进行识别,利用变化矩阵进行城市的变化检测。结果表明:联合像元、深度、对象特征和LightGBM特征选择算法的识别效果最好,平均的总体识别精度达到了88.50%,Kappa系数达到0.86,比基于像元、深度或对象特征的识别方法分别提高了10.50%、15.00%和4.00%;城市变化检测精度达到了87.50%。因此,本文方法是利用甚高分辨率航摄遥感图像进行城市变化的检测的有效方法。     

Coronal index of solar activity VIII, years 1992–1994

The coronal index of solar activity over the period 1992–1994 is given. The data are a good tool to study solar activity, for the Sun as a star, in the solar corona over a solar cycle and its influence in the heliosphere.     

Structure and stability of prominences with helical structure

Observations of internal structure and development of four helical prominences are presented. We assume that the helically twisted fine structure threads are outlining magnetic field lines and we found that it is possible to describe the magnetic fields by the uniform twist configuration, with the twists ranging between 2 and 7. The estimated lower limits for the magnetic fields were about 20 G which give lower limits for the currents flowing along the prominences in the range between 2 × 10¹⁰ A and 2 × 10¹¹ A and current densities at the axis of the prominences about 10^-4 A m^-2. The upper limit of electron drift velocity could be estimated as 1 m s^-1, which is far below the critical velocities for the onset of plasma microinstabilities.The stability of the studied prominences is discussed and the criteria for the onset of eruptive instability are established for a prominence modelled as a twisted and elliptically curved magnetic flux tube which is anchored in the photosphere and affected by its mirror-current. The eruption starts when the prominence attains a critical height which must be larger than half of the footpoint separation and depends on the values of twist, radius, and footpoint distance of the magnetic flux tube. The observed examples of eruptive prominences agree very well with the predictions. Possible applications to the two-ribbon flare process are outlined.Properties of stable cylindrical prominences in equilibrium are analyzed and a criterion for the distinction between the Kuperus-Raadu and Kippenhahn-Schlüter types of prominences is proposed. According to established criteria, two of the studied prominences were of the Kuperus-Raadu type, while the other two were of the Kippenhahn-Schlüter type.     

Vertical transport of polycyclic aromatic hydrocarbons in different particle-size fractions of sandy soils

Vertical transport of selected polycyclic aromatic hydrocarbons (PAHs) in different particle-size fractions of sandy soils was investigated by simulation experiments in soil columns. Tested soil samples were fractionized into three particle-sizes including sand, coarse silt and fine silt (2,000–50, 50–20 and <20 μm). Rainfall simulations were conducted in artificially PAHs contaminated soil columns with 30 cm length and 5 cm diameter in 40 days. PAHs were extracted from soil samples and determined by high performance liquid chromatography (HPLC). Results showed that the residue level of PAHs in fine silt fraction reached 35.85 mg/kg, which was significantly higher than those in sand and coarse silt fraction (16.28 and 11.80 mg/kg, respectively), probably because PAHs in macroporous fractions were prone to volatilize or degrade compared with that in microporous fractions. Linear relationship between the residue levels of individual PAH (R _PAHs) and the value of partition coefficient (log K _oc) was regressed as R _PAHs = 1.55 × log K _oc − 5.86, R ² = 0.91, n = 9. These results indicated that vertical transport of the mixed PAHs in soils were controlled both by the nature of PAHs (i.e. log K _oc, molecular weight), soil particle size and soil organic contents, which could influence the transport of PAHs.     

GPS positioning algorithm for a spinning vehicle with discontinuous signals received by a single-patch antenna

A GPS positioning algorithm is studied and applied to locate a spinning vehicle on which a single-patch antenna is mounted. Because the antenna is directional and the received signal is periodically discontinuous, the bits and frames cannot be synchronized to assemble the transmission time of the satellite signals. The characteristics of the signals received by a single-patch antenna are described. The means by which the tracking loop works with these discontinuous signals are analyzed and simulated. Aiming at spinning projectiles, the positioning algorithm forming differencing with respect to a reference satellite is applied to locate the spinning vehicle by using code phases obtained in the tracking of the discontinuous signals. Experiments were carried out, and the results showed that the positioning algorithm works properly on the spinning vehicle. The results revealed that the positioning error of the algorithm applied to a spinning vehicle is close to that of the conventional positioning method applied to a non-spinning vehicle.