从地理态势分析科索沃战争中的地理环境

给出了地理态势的概念, 初步探讨了地理环境的分析方法, 并从地理态势角度分析了科索沃战争的发生、发展和结局。     

Static compression of the hydrous magnesium silicate phase D to 30 GPa at room temperature

Phase D is a dense hydrous magnesium silicate (ideal formula MgSi₂H₂O₆) which contains silicon cations exclusively in octahedral coordination. Measurements of the unit cell parameters of phase D were made to pressures of 30 GPa using a diamond anvil cell and employing synchrotron X-ray diffraction. A neon pressure medium was used. Using a third order Birch-Murnaghan equation of state the isothermal bulk modulus of phase D was determined as 166(±3) GPa with K′ equal to 4.1(±0.3). The compression of phase D is anisotropic with the c-axis twice as compressible as the a-axis. Above 20 GPa, however, the c/a ratio becomes pressure independent. Received: 29 July 1998/ Revised, accepted: 5 August 1998     

Equations of state of magnesium silicates anhydrous B and superhydrous B

High-pressure single crystal X-ray diffraction experiments of phase anhydrous B and superhydrous B have been carried out to 7.3 and 7.7?GPa, respectively, at room temperature. Fitting a third-order Birch-Murnaghan equation of state to the P-V data yields values of V ₀?=?838.86?±?0.04?ų, K_T,0?=?151.5?±?0.9?GPa and K′?=?5.5?±?0.3 for Anhy-B and V ₀?=?624.71?± 0.03?ų, K_T,0?=?142.6?±?0.8?GPa and K′?=?5.8?±?0.2 for Shy-B. A similar analysis of the axial compressibilities in Anhy-B reveals that the c-axis is most compressible (K_c?=?137?±?3?GPa), the b-axis is least compressible (K_b?=?175?±?4?GPa), and the a-axis is intermediate (K_a?=?148?±?1?GPa). In Shy-B, the a-axis is most compressible (K_a?=?135?±?1?GPa), followed by the b- and c-axes which have similar compressibilities (K_b?=?146?±?3?GPa; K_c?=?148?±?3?GPa). The fact that the b-axis of Shy-B is approximately 16% more compressible than Anhy-B is primarily due to differences in the O-T layer in which the H atoms are located and the linkages with the adjacent O layers. The rigid edge-sharing chains of MgO₆ and SiO₆ octahedra in the O layer control compressibility along the a- and c-axes in both structures. The net result is a reduction in the overall anisotropic compression from ～22% in Anhy-B to ～9% in Shy-B.     

现代测绘教育改革与计算机辅助教学

在阐述测绘高新技术特点和传统会教学方法局性的基础上,分析了计算机辅助教学方法的特点及在现代测绘教育改革中的作用。最后针对现代高等测绘教育提出了一些计算机辅助教学的基本思路。     

《地球学报》2005—2018年主要期刊评价指标变化趋势分析

期刊评价指标能定量评价期刊的相互影响和相互作用,正确评估期刊在科学交流体系中的作用和地位.本文基于2006—2019年版《中国科技期刊引证报告(核心版)》收录的统计数据,选取了《地球学报》期刊被引用计量指标(核心总被引频次、核心影响因子)、期刊来源计量指标(来源文献量、平均引文数、基金论文比)、学科分类内期刊计量指标(综合评价总分、学科扩散指数、学科影响指标),分析了其变化趋势,结论如下:核心总被引频次、平均引文数、学科扩散指数、学科影响指标显著提高;核心影响因子和综合评价总分波动式上升;来源文献量、基金论文比基本保持稳定.上述研究表明,《地球学报》学术质量和影响力不断提升,科学交流程度和吸收外部信息能力显著增强,这与其近年来实施的一系列影响力提升措施密切相关,如注重文章质量和原始创新性,树立精品意识;辟特色栏目,推优秀专辑;独特的封面设计理念及"封面故事";注重编辑与出版质量;关注出版行业和期刊发展动态等.     

高精度水下定位的一种实现方案

提出了一种运用GPS和超短基线等设备实现潜器水下高精度定位的方案,给出了完整的定位解算数学模型,并进行了误差仿真分析。     

苏南块体的深部构造及其油气前景

苏南块体中地壳存在一低速层,Vp约为5.8～6.0km/s,它与地下高导层相对应,电阻率仅4～20Ω·m,是中地壳塑性层的反映;苏南块体属于太平洋型块体,是有利的油气分布区块;它处在地球化学急变带上,壳幔相互作用比较强烈,故该区的油气受深部因素的影响或控制比较明显,是有利的深部无机成因油气分布区。中地壳低速高导层(蛇纹石化橄榄岩)构成油气“发生器”;上地幔则是“原料库”;沉积盆地是“存储器”。当地幔流体中H2缺失或不足时便没有烃生成,只能形成CO2或以CO2为主的气藏。黄桥CO2气藏已被公认是幔源无机成因气体,实质上是由在中地壳进行的不完整费-托合成反应所致。镇江—常州—无锡—苏州—昆山一带为油气富集带,具有深部成因油气的良好远景。     

Global assessment of the European Union fishing fleet: An update

This paper provides a global analysis of recent trends in the EU fishing fleet. Analysis of the capital productivity, labour rates, and economic benefits of the fleet revealed that considerable replacement of fishermen by better technology and well-equipped vessels occurred between 1990 and 2006. The analysis confirms that the Common Fisheries Policy (CFP) has been ineffective in reducing fishing capacity. In addition, the changes in capacity that occurred in this time interval differed among the different sectors of the fleet. Some members of the high sea fishing fleet increased their capacity (range 11–57%), and the deep-sea sector, which has greater tonnage and fishing power, increased its fishing capacity by 34–44%. These results confirm the ineffectiveness of the CFP in reducing overcapacity and illustrate the continuing threat of overcapacity to the long-term sustainability of fishery resources.     

Numerical simulation of flow around a circular cylinder close to a flat seabed at high Reynolds numbers using a k–ε model

High Reynolds number flows around a circular cylinder close to a flat seabed have been computed using a two-dimensional standard high Reynolds number k–ε turbulence model. The effects of gap to diameter ratio, Reynolds number and flat seabed roughness for a given boundary layer thickness of the inlet flow upstream of the cylinder have been investigated. Hydrodynamic quantities and the resulting bedload transport have been predicted, and the vortex shedding mechanisms have been investigated. Predictions of hydrodynamic quantities around a cylinder located far away from the bed (so that the effect of the bed is negligible) are in satisfactory agreement with published experimental data and numerical results obtained for the flow around an isolated cylinder. Results for lower Reynolds number flows have also been computed for comparison with the high Reynolds number flow results. Overall it appears that the present approach is suitable for design purposes at high Reynolds numbers which are present near the seabed in the real ocean.     

Analysis of the simulated climatic characters of the South Asia High with a flexible coupled ocean-atmosphere GCM

The ability of a climate model to reproduce the climatic characters of the South Asia High （SAH） is assessed by analyzing the 110-yr output of a Flexible Coupled GCM, version 0 （FGCM-0）. Comparing the results of FGCM-0 with the NCEP/NCAR reanalysis data, the major findings show that FGCM-0 has better results in simulation of the geopotential height field at 100 hPa, and reproduces fairly the main atmospheric circulation centers. However, there are still some differences in the simulated results compared with the reanalysis data. The coupled model also successfully reproduces the mean seasonal variation of the SAH, that is, it moves from the Pacific Ocean to the Asian continent, remaining over the Tibetan Plateau from winter to summer, and then withdraws from the Tibetan Plateau to the Pacific Ocean from summer to winter. However, such observed relationships between the SAH positions and the summer precipitation patterns cannot be fairly reproduced in the FGCM-0.