软土深基坑变形与控制技术初探

通过对软土深基坑变形机理与影响因素的分析,提出了基坑工程变形全过程控制的理念,探讨了控制变形的设计与施工技术方法及针对变形异常应采取的应急措施。结合工程实践,分析了软土深基坑变形的特征,应用地层损失法原理计算了墙后地表沉降量,与实测值比较,得出了该方法可以应用于工程实践的认识。     

黄东海浮游生物群落呼吸率对碳平衡的重要性

黄东海接受长江冲淡水和黑潮带来的大量营养盐和有机物质,其碳循环对陆架海碳源汇格局至关重要.浮游生物群落呼吸是影响碳循环的重要过程.为揭示黄东海浮游生物群落呼吸率(PCR)对碳平衡的贡献,于2011年四季使用黑白瓶培养法测定黄海南部及东海北部浮游群落呼吸率和初级生产力,并同步测定温度、盐度、营养盐、叶绿素和细菌丰度等环境...     

东海油气资源区海底沉积物的工程地质特征

根据2001年6月的航次调查及随后的沉积物样品的试验室分析资料,从物理性质和力学特征各方面对东海油气资源区海底沉积物进行了综合工程地质特征研完。发现本区沉积物结构、剪切特征、含水量和液塑限随深度的变化而变化;本区海底沉积物类型既分布有中砂、细砂和粉砂3种砂性土,也分布有扮质粘土、淤泥质粘土和粘质扮土3种粘性土,沉积物的物理力学性质与相立的土类性质相一致。     

埕岛油田海域海底沉积特征与工程地质特性

详细阐述了埕岛油田海域海底沉积和冲淤特征,介绍了沉积物的成分、类型和分布特征,并综合描述了埕岛海域海底地貌形态和海底沉积物的物理力学特性,上述研究对埕岛油田的进一步研究和开发有指导意义。     

河流入海物质通量对海、陆环境变化的响应

入海河流物质通量研究是陆—海相互作用和全球海洋通量联合研究计划的重要命题。我国是最早开展物质通量研究的国家之一。自20世纪90年代以来,国家自然科学基金项目和国家重大基础研究计划项目都开展了有关河流和边缘海物质通量的研究,即将开始的全国海岸带环境调查专项也把主要河流物质入海通量及其海洋环境效应研究作为主要内容之一。根据当前国内外河流物质通量研究的最新进展,较系统地阐述了河流入海物质通量的概念和对邻近大陆和海洋环境变化的响应。并在此基础上强调指出,河流入海物质通量是研究陆—海相互作用及其全球变化效应的重要参量。归纳了河流入海物质通量研究中需要解决的关键问题。     

强弱南海夏季风年广西的天气及预测概念模型

利用南海季风试验研究(1997～2000)的成果资料,对强弱南海夏季风年广西的天气作了对比研究,主要分析了雨季开始、年雨量分配及丰欠、热带气旋活动特点等方面的差异并归纳出一个简单的预测概念模型,可供业务工作者在制作年景预测上参考。     

胶西北地区三维地质模型构建及意义

为服务于山东深部找矿,结合金矿成矿机理及预测评价,利用Creatar Xmodeling平台建立了胶西北地区三维地质模型,直观、清楚地反映出胶西北地区地层厚度及变化趋势,岩浆岩展布规模、深度及相互接触关系,从空间分布视角可以看出,金成矿与玲珑花岗岩、郭家岭花岗岩、伟德山花岗岩存在密切关联;全方位展示出断裂带之间的关系,...     

Deep Space 1 at comet 19P/Borrelly: Magnetic field and plasma observations

On September 22, 2001 the Deep Space 1 spacecraft performed a flyby at comet 19P/Borrelly at a solar distance of 1.36 AU leading the Earth by 74^° in longitude. The spacecraft-comet distance at closest approach was 2171 km. The bow shock had a magnetic compression ratio of 2.5 at a distance of 147 100 km from the nucleus. Deep Space 1 first entered the sheath region essentially from the north polar region. Fluctuations from the cometary ion pickup were present throughout the sheath region and even well upstream of the shock, as expected. The magnetic field pileup region had a peak field strength of 83 nT and was shown to be consistent with a pressure equal to the solar wind ram pressure. The peak field location was offset from the time of closest approach. It is uncertain whether this is a spatial or temporal variation. Draping of magnetic fields around the nucleus was sought, but evidence for this was not apparent in the data. A possible explanation is that the interplanetary solar wind was composed of turbulent short-scale fields, and thus the fields were not symmetric about the point of closest approach. During the flyby phase there were in general few intervals of ACE data where there were large scale Parker spiral fields. With the addition of plasma data, the shock properties are investigated. The characteristics of magnetic draping, pileup and fluctuations are explored. These comet 19P/Borrelly results are contrasted with other cometary flyby results.     

The physical structures of snow and sea ice in the Arctic section of 150°-180°W during the summer of 2010

The physical structures of snow and sea ice in the Arctic section of 150°-180°W were observed on the basis of snow-pit, ice-core, and drill-hole measurements from late July to late August 2010. Almost all the investigated floes were first-year ice, except for one located north of Alaska, which was probably multi-year ice transported from north of the Canadian Arctic Archipelago during early summer. The snow covers over all the investigated floes were in the melting phase, with temperatures approaching 0℃ and densities of 295-398 kg/m3 . The snow covers can be divided into two to five layers of different textures, with most cases having a top layer of fresh snow, a round-grain layer in the middle, and slush and/or thin icing layers at the bottom. The first-year sea ice contained about 7%-17% granular ice at the top. There was no granular ice in the lower layers. The interior melting and desalination of sea ice introduced strong stratifications of temperature, salinity, density, and gas and brine volume fractions. The sea ice temperature exhibited linear cooling with depth, while the salinity and the density increased linearly with normalized depth from 0.2 to 0.9 and from 0 to 0.65, respectively. The top layer, especially the freeboard layer, had the lowest salinity and density, and consequently the largest gas content and the smallest brine content. Both the salinity and density in the ice basal layer were highly scattered due to large differences in ice porosity among the samples. The bulk average sea ice temperature, salinity, density, and gas and brine volume fractions were-0.8℃, 1.8, 837 kg/m3 , 9.3% and 10.4%, respectively. The snow cover, sea ice bottom, and sea ice interior show evidences of melting during mid-August in the investigated floe located at about 87°N, 175°W.