大兴安岭闪电时空分布特征分析

利用大兴安岭林区2005—2006年闪电定位系统监测资料,分析了该地区地闪的月变化、日变化、闪电密度的时空分布特征。结果表明:大兴安岭林区闪电的月变化呈单峰分布,6—8月是闪电多发期;日变化呈双峰分布,夏季14时和19时是该地区强对流天气最易发展成熟的时段;莫尔道嘎林区是闪电频发的中心地带。从雷击火发生的时空分布得出北部原始林区是雷击火多发区域。     

河南省近年来遥感监测的森林火灾时空分布规律分析

森林火灾作为一种自然灾害,其发生原因不仅来自于自然因素,从众多的火灾调查中发现,更多地来自于人类活动因素,其发生的时空分布特点和规律,受自然和人类活动共同影响.对2003-2008年春、冬季(11月-次年4月)河南省森林防火期内遥感监测并已查明的森林火灾进行统计分析,结果发现:河南省森林火灾近年来有逐年增多的趋势;冬、春之交的3月为森林火灾的高发月份;从火灾的日变化规律来看,12-15时为一天中森林火灾的高发时段;从火灾发生的空间分布来看,伏牛山南麓发生森林火灾的频率较高.     

浙西南山区热带气旋降水的时空分布特征

对影响丽水热带气旋进行时空分布特征研究,1950 ～ 2010年 61年间,影响丽水的热带气旋共有119个,年均1.95个,在月分布上呈单峰型分布,7～9月是丽水受热带气旋影响的高峰期,同时,从影响丽水热带气旋的降水强度和影响丽水热带气旋的降水等级也说明,7～9 月是丽水受热带气旋降水影响最重的月份,且特别严重影响的热...     

辽宁雾预报区的划分初探

分析了1997—2006年辽宁境内能见度小于1000 m雾的时空分布特征。结果表明：就雾发生的频率而言,辽宁存在两个高值区和两个低值区,高值区分别位于黄海北部沿岸至辽宁东部山区和锦州北部至阜新一带,低值区分别位于辽宁中北部平原以及朝阳地区。从雾的日变化上看,近86%的雾出现在夜间,近69%的雾出现在02-08时,且多为辐射雾。地域不同但气候条件相近时,雾的日变化与雾发生的次数存在极其相似的特点。依据相似的地理环境和气候条件、雾的日变化特征以及雾发生次数等,将辽宁划分为5个预报区,对雾采取分区预报,以提高雾预报的准确率。     

广东灰霾天气预警指标及时空分布

霾,也称灰霾,香港澳门一带称之为烟霞,是指悬浮在大气中的大量微小尘粒、烟粒、硫酸与硫酸盐、硝酸与硝酸盐、有机碳氢化合物等化学物质微粒的非水成物组成,导致大气浑浊、视野模糊、水平能见度〈10km的气溶胶系统。目前我国有4个灰霾严重地区：黄淮海地区、长江河谷、四川盆地和珠江三角洲。     

中心城区地表温度空间分布及地物降温效应——以南京市为例

基于TM图像,采用灰度图像分割算法,自动提取南京市中心城区的不透水面、植被及水体;并用单窗算法反演了地表温度;依据离市中心的距离将中心城区分为45级缓冲区,依次统计分析每一级缓冲区内的平均温度、不透水面温度、植被温度、水体温度及各类地物的面积比例等;建立了地表温度与不透水面比例、植被比例、水体比例之间的关系模型.研究结果表明:随离市中心距离的增大,地表温度降低;植被、水体具有降温效应,水体的降温效应是植被的2.43倍;地表温度与不透水面比例、植被比例、水体比例的综合关系模型模拟效果较好.     

小白洋淀水-沉积物系统多环芳烃的分布、来源与生态风险

以端村小白洋淀为研究对象,利用GC-MS测定了6个样点水、悬浮物和沉积物中15种优控多环芳烃(PAHs)的含量,分析了其组成与来源特征,探讨了不同多环芳烃单体的生态风险,结果表明:(1)15种优控多环芳烃的总含量(PAH15),水相为40.1-74.0ng/L,算术均值51.0ng/L;悬浮物为2438.0-5927.0ng/g,算术均值4528ng/g;沉积物为466.9-1366.4ng/g,算术均值为755.6ng/g;与国内外有关研究相比,污染较轻,(2)三相中均以2、3环PAHs为主,其比例均高于80%;并且,从水相、悬浮物相到沉积物相,2环PAHs依次降低,3环、4环依次升高,高环检出率和含量也依次升高,(3)沉积物中多环芳烃的来源以生物质燃料(秸秆、薪材)和煤的燃烧为主,以液体化石燃料(汽油、柴油和原油)的燃烧为辅,(4)沉积物中的芴(FLO)、菲(PHE)含量在潜在生态风险效应区间低值(ERL)与中值(ERM)之间,其生态风险几率介于10%-50%之间;其他PAHs单体的含量均低于ERL,其生态风险几率均低于10%.     

Global sea level change and thermal contribution

The global long-term sea level trend is obtained from the analysis of tide gauge data and TOPEX/Poseidon data. The linear trend of global mean sea level is highly non-umiform spatially, with an average rate of 2.2 mm year-1 in T/P sea-level rise from October 1992 to September 2002. Sea level change duc to temperature vanation (the thermosteric sea level) is discussed. The results are compared with TOPEX/Poseidon altimeter data in the same temporal span at different spatial scales. It is indicated that the ther-mal effect accounts for 86% and 73% of the observed seasonal variability in the northern and southern hemispheres, respectively. The TOPEX/Poseidon observed sea level lags behind the TSI, by 2 months in the zonal band of 40°-60° in both the northern and southern hemispheres. Systematic differences of about 1-2cm between TOPEX/Poseidon observations and thermosteric sea level data are obtained. The potential causes for these differences include water exchange among the atmosphere, land, and oceans, and some pos-sible deviations in thermosteric contribution estimates and geophysical corrections to the TOPEX/Poseidon data.     

Thickness distribution and extent of sea ice and snow in Prydz Bay and surrounding waters observed in 2012/2013 austral summer

Three ship-based observational campaigns were conducted to survey sea ice and snow in Prydz Bay and the surrounding waters(64.40°S–69.40°S, 76.11°E–81.29°E) from 28 November 2012 to 3 February 2013. In this paper, we present the sea ice extent and its variation, and the ice and snow thickness distributions and their variations with time in the observed zone. In the pack ice zone, the southern edge of the pack ice changed little, whereas the northern edge retreated significantly during the two earlier observation periods. Compared with the pack ice, the fast ice exhibited a significantly slower variation in extent with its northernmost edge retreating southwards by 6.7 km at a rate of 0.37 km?d-1. Generally, ice showed an increment in thickness with increasing latitude from the end of November to the middle of December. Ice and snow thickness followed an approximate normal distribution during the two earlier observations(79.7±28.9 cm, 79.1±19.1 cm for ice thickness, and 11.6±6.1 cm, 9.6±3.4 cm for snow thickness, respectively), and the distribution tended to be more concentrated in mid-December than in late November. The expected value of ice thickness decreased by 0.6 cm, whereas that of snow thickness decreased by 2 cm from 28 November to 18 December 2012. Ice thickness distribution showed no obvious regularity between 31 January and 3 February, 2013.