关于高层建筑防侧击雷等电位连接圆钢用材规格的探讨

利用《建筑物防雷设计规范》(GB 50057—2010)中的雷击距理论公式和热力学中的有关焦耳定律公式,计算了侧击雷的雷电流特征及侧击雷防护等电位连接圆钢用材规格,分析探讨了等电位连接圆钢用材规格随建筑高度的变化关系。结果表明:建筑物高度越高,遭受的侧击雷电流幅值也越大;随着建筑高度的增加,防侧击雷等电位连接所需最大圆钢直径也将增大,它们之间基本呈线性增长关系。本文的研究结果可为高层建筑侧击雷防护节省圆钢用材提供理论指导。     

一维水质模型结合改进的输出系数法在流域非点源污染负荷估算中的应用

非点源污染是导致流域水体水质恶化的关键污染来源之一,为了估算流域非点源污染负荷,本文提出将一维水质模型应用于分离监测断面点源污染负荷和非点源污染负荷的方法,并结合了改进的输出系数法,以COD_Mn和NH₃-N为代表性指标,将该模型应用于潮河下游流域,并与传统的水文分割法结合改进的输出系数法估算非点源污染负荷的结果进行对比。结果表明,一维水质模型结合改进的输出系数法估算流域非点源COD_Mn和NH₃-N污染负荷模拟值的纳什系数均在0.800以上,具有良好的模拟精度,同时避免了水文分割法无法较好地模拟枯水期非点源污染负荷的弊端。该方法在运用SWAT（soil and water assessment tool）模型预测得到水文数据的情况下,能够预测流域非点源污染负荷,作为SWAT模型对COD模拟的补充。     

河南省一次致灾强对流天气的中尺度分析

利用常规观测资料、中尺度分析产品和雷达资料对2013年8月1日凌晨发生在河南省西部、北部的一次致灾强对流天气过程进行分析.结果表明:这次强对流是在上干冷下暖湿的不稳定大气层结条件下产生的,较大的垂直风切变出现在强对流发生后,可能与强对流天气产生时间较晚有关;地面辐合线是这次强对流产生的触发机制,强对流发生在地面等温线和等露点线的密集区内.云图亮温的低值中心对应地面的强雨区.1日凌晨,对流回波东移加强,先后形成的两条弓形回波,均存在明显的低层弱回波区和中高层的悬垂回波结构,大风发生在弓形带状回波后侧;对流回波带低层有很强的西南风急流,使得强对流回波形成弓形带状回波;强回波带的前沿速度场上,有中尺度辐合线、辐合区、逆风区存在,它们的出现和维持是产生局地强降水的一个有用指标,中尺度系统的存在是强对流风暴产生、维持、发展的必要条件;较大垂直液态含水量的维持为产生强降水提供了有利条件,垂直液态含水量的增减,预示着地面强对流天气的开始和减弱.     

白令海陆架区夏季水文分布特征及年际变化

On the basis of the CTD data obtained within the Bering Sea shelf by the Second to Sixth Chinese National Arctic Research Expedition in the summers of 2003, 2008, 2010, 2012 and 2014, the classification and interannual variation of water masses on the central Bering Sea shelf and the northern Bering Sea shelf are analyzed. The results indicate that there are both connection and difference between two regions in hydrological features. On the central Bering Sea shelf, there are mainly four types of water masses distribute orderly from the slope to the coast of Alaska: Bering Slope Current Water(BSCW), MW(Mixed Water), Bering Shelf Water(BSW) and Alaska Coastal Water(ACW). In summer, BSW can be divided into Bering Shelf Surface Water(BSW_S) and Bering Shelf Cold Water(BSW_C). On the northern Bering Sea shelf near the Bering Strait,it contains Anadyr Water(AW), BSW and ACW from west to east. But the spatial-temporal features are also remarkable in each region. On the central shelf, the BSCW is saltiest and occupies the west of 177°W, which has the highest salinity in 2014. The BSW_C is the coldest water mass and warmest in 2014; the ACW is freshest and mainly occupies the east of 170°W, which has the highest temperature and salinity in 2012. On the northern Bering Sea shelf near the Bering Strait, the AW is saltiest with temperature decreasing sharply compared with BSCW on the central shelf. In the process of moving northward to the Bering Strait, the AW demonstrates a trend of eastward expansion. The ACW is freshest but saltier than the ACW on the central shelf,which is usually located above the BSW and is saltiest in 2014. The BSW distributes between the AW and the ACW and coldest in 2012, but the cold water of the BSW_C on the central shelf, whose temperature less than 0°C, does not exist on the northern shelf. Although there are so many changes, the respond to a climate change is synchronized in the both regions, which can be divided into the warm years(2003 and 2014) and cold years(2008, 2010 and 2012). The year of 2014 may be a new beginning of warm period.     

南极普里兹湾暖水涌升陆架过程及在陆架上的时空分布特征分析

Hydrographic observations collected by conductivity-temperature-depth(CTD) and instrumented elephant seals on the Prydz Bay continental shelf during 2012 and 2013 are used to characterize the intrusion of modified circumpolar deep water.As a regular occurrence,modified circumpolar deep water(MCDW) intrudes onto the shelf mainly between 150–300 m layer of 73°–75°E and then turns southeast affected by the cyclonic gyre of the Prydz Bay.The southernmost point of the warm water signal is captured on the east front of Amery Ice Shelf during March 2012.In terms of vertical distribution,MCDW occupies the central layer of 200 m with about 100 m thickness in the austral summer,but when to winter transition,the layer of MCDW deepens with time on the central shelf.     

不同CTD数据垂向分辨率对黑潮地转流动力计算的影响分析

基于日本海洋信息中心提供的东海黑潮PN断面垂向分辨率不同的2种CTD数据,采用动力高度法计算了2000—2011年的断面流速。通过对49个航次的流场结构、最大流速、流幅、流量等黑潮特征值的对比,分析了不同数据垂向分辨率对黑潮地转流动力计算的影响。结果表明:数据垂向分辨率不同对东海黑潮的流量几乎没有影响,对平均流幅影响很小,对流核位置略有影响,但对平均流核个数、平均最大流速影响较大。2种数据对应的流场差异主要有:与低分辨率数据对应的流场相比较,高分辨率数据对应的流场流核区流速较大、平均流核数偏多。不同流核结构在2种数据对应的流场中出现概率差别较大,低分辨率数据结果中的单核结构出现概率最高,高分辨率数据结果中的双核结构出现概率最高。     

黏性土包气带中流体迁移规律

以黏土模拟低渗透包气带环境,探究了混溶流体在包气带中的迁移规律。实验结果表明:混溶流体在横向和垂向的最大迁移距离与流体泄漏量均符合幂函数变化规律y=axb。随着流体注入体积的增加,横向和垂向迁移距离不断增大,迁移速率逐渐减小。文章提出以横纵比作为反映流体在包气带中迁移变化规律的重要指标。横纵比总体呈下降趋势,具体分为两个阶段:流体注入体积为0~3 046 m L时,横纵比呈先上升后稳定的趋势,横纵比大于1。此阶段流体以横向发育为主,污染羽剖面呈扁平状椭圆;当流体注入体积大于3 046 m L,横纵比逐渐减小到1以下并持续减小。此阶段流体以垂向发育为主,污染羽剖面逐渐转变为竖直长条状椭圆。     

印度洋-太平洋暖池季节变化及其相应的大气环流形式

首先通过对英国大气科学数据中心海表面温度资料和Levitus随深度变化的海温资料的分析,给出了印度洋-太平洋暖池季节变化的详细描述.另外,利用NCEP/NCAR再分析大气资料中的风场数据,采取将水平风场分量分解为无辐散分量和无旋分量的方法,分析了相应于暖池季节变化的大气环流形式.得到了这样的结论：第一,印度洋-太平洋暖池的位置随季节变化南北移动;暖池面积在北半球的5月和9月达到两个极大值;无论就海表面温度还是深度而言,该暖池分别存在一或两个强度中心.第二,尽管印度洋-太平洋暖池中间被南亚大陆所间隔,但是暖池上空对流层大气运动对于暖池的季节变化却是作为一个整体响应的.     

Comparison of TOPEX/POSEIDON altimeter derived wave period with ocean buoy data in the East China Sea and South China Sea

Altimeter wave period data obtained from continental shelf seas are analyzed in this paper. Empirical models are introduced for zero up-crossing and peak wave period calculation with TOPEX/POSEIDON data. Their performances are assessed using independent validation dataset in four sites in the open ocean of China. To provide more accurate wave period estimation, new coefficients are applied to reliable in situ data. Comparison of our estimated the wave periods with new linear calibrations based on independent data of Seapac 2100 deployed in the East China Sea and South China Sea showed that the accuracy was improved over estimates determined from earlier empirical models. Regional analysis indicated that the wave period model works better under wind sea condition.