一次飑线风暴的环境条件和雷达回波特征分析

利用常规气象观测和新一代天气雷达监测资料,对大兴安岭地区加格达奇市2006年8月一次飑线天气的环境条件和雷达回波特征等分析发现：此次过程的影响系统高空槽为前倾结构,飑线发生在地面冷锋前,大气具有较强的不稳定层结,有利于上升运动,水汽充足,低层较强的垂直风切变使对流云团和弓形等线状回波生成并较长时间地维持和发展。对流云团位置与上升运动区域较为一致,产生飑线的强对流云团出现在中低层垂直速度梯度较大并靠近上升运动中心一侧,并位于低层比湿和水汽通量散度梯度较大区域即干锋附近以及K指数能量锋上。飑线弓形回波出现在一个中尺度椭圆状对流云团中心内部发展最强处。当云团向东北偏东方向移过加格达奇雷达站时,雷达反射率因子先后呈现出弓形、＂人＂字形等线状回波特征,当线状回波南端＂人＂字形顶部较强回波和后侧入流急流前方＂V＂型槽口的尖峰移经加格达奇时,带来了雷雨大风天气。     

2013—2017年夏季东北冷涡下东北地区MCS的统计特征

利用2013—2017年6—8月FY-2E和FY-2G地球静止卫星相当黑体温度（Black Body Temperature,TBB）资料、NCEP/NCAR再分析资料,对我国夏季东北冷涡下东北地区MCS的分布和活动特征进行了统计分析,结果表明：（1） MCS的活动具有明显的月际变化和日变化特征,6月对流活动最活跃。MCS的主要移向是东、东北和东南,平均移动距离3.99个经纬距。（2） MCS成熟时刻的面积、偏心率和生命史均小于江淮地区以及中国中东部,云顶高度低于江淮地区,整个生命史表现出发展快消亡慢的特征,与江淮地区相反。（3）基于MCS的定义得到的Z标准,对2016—2017年的MCS作了统计分析并与J标准统计得到的MCS进行对比,得出,两种定义下的MCS环境场特征基本一致,主要表现为MCS多生成于500 hPa槽前和槽后,对流层高层MCS位于双急流之间靠近北支急流的辐散区,南侧急流高度在200 hPa,北侧的急流高度在250 hPa。低层,位于低空急流左侧,低涡南侧、东南侧,有较强的水汽和动量输送。槽前生成的MCS南侧中层存在垂直反环流向MCS输送干暖空气与位涡,槽后生成的MCS两侧均有大值位涡向其输送,同时北侧冷干空气的输送使锋区及上升运动加强,更有利于MCS的形成。（4）两种标准下的MCS造成的降水明显不同,在统计强降水方面Z标准要优于J标准。由于Z标准空间与时间尺度较小,统计得到的MCS较多;但同时会遗漏部分相对弱的MCS。     

亚洲急流与冬季风的关系及其对中国气候的影响

利用NCEP\NCAR逐月再分析资料和中国台站逐日观测数据,采用奇异值分解(SVD)、相关分析和合成分析等方法,研究冬季亚洲高空急流的配置与冬季风的关系及其对地面气候的影响.结果表明,青藏高原至亚洲东部沿海的副热带急流强(弱),高纬的温带急流弱(强)时,中国中、东部大范围地区气温偏低(高);中东急流强(弱),东亚副热带急流偏南(北),温带急流东南部较弱(强)时,西南气温偏低(高),东北气温偏高(低),中、东部地区冬季降水偏多(少).结合水平风场的变化,副热带地区出现西风异常弱,温带出现东风异常时,有利于东亚大槽加深并向南扩张,低层偏北风加强,东亚冬季风增强,而青藏高原反气旋环流被削弱,冷高压减弱,相应的高原季风减弱.高、低纬急流区纬向风的差异较大时,加强了急流对低层冷、暖空气交绥的引导和汇聚的作用.东亚季风指数(EAMI)与高原季风指数(PMI)在冬季多呈负相关.冬季风异常期间,若副热带急流偏强,温带急流偏弱,高纬的干冷空气受南侧急流的汇聚作用而南侵,有利于中国大部分地区降温,降水减少;反之,低纬的暖湿气流受到北侧急流引导而向北输送,导致中国大部分地区升温,降水偏多.     

辐射板强化喷管换热与红外抑制效果试验研究

试验研究了在发动机喷管中加装金属辐射板前后,喷管壁面温度、热喷流温度与喷管红外辐射特征的变化。结果表明,加装金属辐射板后,热喷流与喷管壁面之间的热量传递显著增强,热喷流中心温度降低,壁面温度明显升高,在90°方向上,热喷流3～5μm波段的红外辐射强度降低了38.5%。文中从热喷流、喷管壁面以及金属辐射板等相关部件的温度变化情况对红外辐射强度的变化原因进行了解释。      

Comparative application of two mathematical models to predict sedimentation in Yermasoyia Reservoir,Cyprus

The Yermasoyia Reservoir is located northeast of the town of Limassol, Cyprus. The storage capacity of the reservoir is 13·6 × 10⁶ m³. The basin area of the Yermasoyia River, which feeds the reservoir, totals 122·5 km². This study aims to estimate the mean annual deposition amount in the reservoir, which originates from the corresponding basin. For the estimate of the mean annual sediment inflow into the reservoir, two mathematical models are used alternatively. Each model consists of three submodels: a rainfall‐runoff submodel, a soil erosion submodel and a sediment transport submodel for streams. In the first model, the potential evapotranspiration is estimated for the rainfall‐runoff submodel, and the soil erosion submodel of Schmidt and the sediment transport submodel of Yang are used. In the second model, the actual evapotranspiration is estimated for the rainfall‐runoff submodel, and the soil erosion submodel of Poesen and the sediment transport submodel of Van Rijn are used. The deposition amount in the reservoir is estimated by means of the diagram of Brune, which delivers the trap efficiency of the reservoir. Daily rainfall data from three rainfall stations, and daily values of air temperature, relative air humidity and sunlight hours from a meteorological station for four years (1986–89) were available. The computed annual runoff volumes and mean annual soil erosion rate are compared with the respective measurement data. Copyright © 2006 John Wiley & Sons, Ltd.     

Radio‐tracking gravel particles in a large braided river in New Zealand: a field test of the stochastic theory of bed load transport proposed by Einstein

Hans A. Einstein initiated a probabilistic approach to modelling sediment transport in rivers. His formulae were based on theory and were stimulated by laboratory investigations. The theory assumes that bed load movement occurs in individual steps of rolling, sliding or saltation and rest periods. So far very few attempts have been made to measure stochastic elements in nature. For the first time this paper presents results of radio‐tracing the travel path of individual particles in a large braided gravel bed river: the Waimakariri River of New Zealand. As proposed by Einstein, it was found that rest periods can be modelled by an exponential distribution, but particle step lengths are better represented by a gamma distribution. Einstein assumed an average travel distance of 100 grain‐diameters for any bed load particle between consecutive points of deposition, but larger values of 6·7 m or 150 grain‐diameters and 6·1 m or 120 grain‐diameters were measured for two test particle sizes. Together with other available large scale field data, a dependence of the mean step length on particle diameter relative to the D₅₀ of the bed surface was found. During small floods the time used for movement represents only 2·7% of the total time from erosion to deposition. The increase in percentage of time being used for transport means that it then has to be regarded in stochastic transport models. Tracing the flow path of bed load particles between erosion and deposition sites is a step towards explaining the interactions between sediment transport and river morphology. Copyright © 2001 John Wiley & Sons, Ltd.     

THE EROSIONAL PROCESS OF THE SOFT SHORE OF CHINA IN THE RECENT DECADES

ＴＨＥ ＥＲＯＳＩＯＮＡＬ ＰＲＯＣＥＳＳ ＯＦ ＴＨＥ ＳＯＦＴ ＳＨＯＲＥ ＯＦ ＣＨＩＮＡ ＩＮ ＴＨＥ ＲＥＣＥＮＴ ＤＥＣＡＤＥＳ ＷａｎｇＷｅｎｈａｉ（王文海）；ＷｕＳａｎｇｙｕｎ（吴桑云）；ＸｉａＤｏｎｇｘｉｎｇ（夏东兴）（ＦｉｒｓｔＩ...     

Modelling of sediment dynamics in a laboratory‐scale experimental catchment

The variability of hillslope form and function is examined experimentally using a simple model catchment in which most landscape development parameters are either known or controlled. It is demonstrated that there is considerable variability in sediment output from similar catchments, subjected to the same hydrological processes, and for which the initial hillslope profiles are the same. The results demonstrate that, in the case of catchments with a linear initial hillslope profile, the sediment output is initially high but reduces through time, whereas for a concave initial profile the sediment output was smaller and relatively constant. Concave hillslope profiles also displayed reduced sediment output when compared with linear slopes with the same overall slope. Using this experimental model catchment data, the SIBERIA landscape evolution model was tested for its ability to predict temporal sediment transport. When calibrated for the rainfall and erodible material, SIBERIA is able to simulate mean temporal sediment output for the experimental catchment over a range of hillslope profiles and rainfall intensities. SIBERIA is also able to match the hillslope profile of the experimental catchments. The results of the study provide confidence in the ability of SIBERIA to predict temporal sediment output. The experimental and modelling data also demonstrate that, even with all geomorphic and hydrological variables being known and/or controlled, there is still a need for long‐term stream gauging to obtain reliable assessments of field catchment hydrology and sediment transport. Copyright © 2005 John Wiley & Sons, Ltd.     

Spatial analysis of the impact of land-use on surface runoff and soil erosion-a case study of western Jilin

IntroductionNever before hasit beensotrue than now,thatlandis ali mitedresource.Population growth and as-sociated human activities,especially agricultureacross the world have not only led to land degrada-tion,but soil loss at rates that have pushed arablesoils to frontier thresholds.In the absence of arablesoil,the human environment would cease to groworeven demise(Ramet al.,2006).Studies haveshownthat in many regions of the world,runoff andsoil erosion differ withland-use type.Judson(1965)re…     

Imaging Borrelly

The nucleus, coma, and dust jets of short-period Comet 19P/Borrelly were imaged from the Deep Space 1 spacecraft during its close flyby in September 2001. A prominent jet dominated the near-nucleus coma and emanated roughly normal to the long axis of nucleus from a broad central cavity. We show it to have remained fixed in position for more than 34 hr, much longer than the 26-hr rotation period. This confirms earlier suggestions that it is co-aligned with the rotation axis. From a combination of fitting the nucleus light curve from approach images and the nucleus' orientation from stereo images at encounter, we conclude that the sense of rotation is right-handed around the main jet vector. The inferred rotation pole is approximately perpendicular to the long axis of the nucleus, consistent with a simple rotational state. Lacking an existing IAU comet-specific convention but applying a convention provisionally adopted for asteroids, we label this the north pole. This places the sub-solar latitude at ∼60° N at the time of the perihelion with the north pole in constant sunlight and thus receiving maximum average insolation.