中国地区高空气象探测气球空间漂移分析

利用中国120个探空站2004年08时所有探空气球漂移信息,结合NCEP再分析场,分析规定等压面上的时空漂移规律,重点选择100、500与925 hPa等压面,采用1、4、7、10月分别代表冬季、春季、夏季、秋季4个季节。初步分析表明;气球的漂移方向主要是受大气环流影响,不同季节中国受不同的系统影响,导致漂移的方向差异明显,夏季以西南漂移为主,冬季、春季与秋季以西北漂移为主,但是在100 hPa以上4个季节均以西南漂移为主,以冬季的漂移距离最大,漂移距离超过120km,夏季最小,约为40 km,春、秋季次之,接近70 km。漂移距离的差异东部比西部显著;沿经圈漂移以向南为主,冬、春与秋季沿经圈漂移以向南为主,春季漂移最大,超过5 km;冬、秋季节漂移距离分别超过3与2 km,夏季沿经圈漂移受大尺度环流影响,200 hPa以下向北漂移,最远漂移超过1 km,200 hPa以上转向南漂移,最远漂移达3 km;沿纬圈以向东为主,以冬季最大,达77 km,夏季最小,接近13 km,春、秋季次之,分别达49和46 km;沿纬圈漂移量要大于沿经圈漂移量,沿纬圈漂移全年平均接近60 km,沿经圈漂移量全年平均接近3.5 km,有量级上的差别;从低层到高层漂移量呈增大趋势,漂移大的范围随高度往西扩张;探空漂移的整体分布范围较大,并且比较均匀。同时还选取了个例分析低空急流条件下探空漂移,结果显示对于中小尺度天气系统不可忽略。     

中国探空气球水平漂移总体特征分析

利用2003年4月至2008年8月全国119个探空台站采集的气球漂移信息,分析了中国探空资料水平漂移距离、漂移距离标准差以及漂移方向的分布特征。研究表明:各层探空气球的漂移距离冬季明显大于夏季;一般探空气球的漂移距离随探空高度的增加而增大,但在夏季南方地区由于风向随高度的反转会出现探空气球水平漂移距离随高度减小的状况。探空气球水平漂移距离的标准差随高度增加而增大,且其大值区分布基本上与水平漂移距离的大值区分布一致。从气球漂移方向上看,冬季的情况相对简单,全国各探空台站各层的漂移方向基本以向东为主;但夏季探空气球漂移的方向比较复杂,在对流层低层,全国各台站漂移方向基本以向东为主,而在对流层高层和平流层,北方地区漂移方向基本向东,而南方地区以向西为主。     

济宁工商银行机房零—地电压问题探讨

首先从7个方面阐明了零一地电压高的可能因素,对济宁市工商银行计算机房零一地电压过高的原因进行了分析,用电路图分析零-地电压高的理论因素,通过电路图分析使用隔离变压器以后零-地电压接近于零的原因,并逐一排除,从而找出导致济宁工商银行零-地电压高的原因为UPS的供电问题,并提出解决方案.     

探空气球漂移特征及对三角形法计算散度的影响

利用2006—2013年南京站、安庆站和杭州站探空资料,讨论华东地区探空气球的漂移特征。设计不考虑气球漂移、考虑全部气球漂移和考虑部分气球漂移3个试验,比较3种情况下三角形法计算的散度差异。结果表明:气球漂移主要受大气环流及其变化影响,纬向上7月和8月气球随高度增加,先向东漂移、后向西漂移,其他月份以向东漂移为主,冬季漂移距离大;经向上受季风影响明显。考虑全部和部分气球漂移与不考虑气球漂移的散度对比表明,平均绝对偏差各月在对流层顶附近均有极大值;相对偏差季节分布明显,前者在6—9月较大,极大值略大于7%,后者冬季大,1月在200 hPa达到25%,在50 hPa超过50%。因此,利用三角形法计算散度所在层次较高或所使用资料中传统探空和特种探空并存时,均需考虑气球漂移影响。     

加法幂等半环上幂零矩阵的特征

根据主子式、主对角元、幂零指数以及伴随矩阵给出了加法幂等半环上幂零矩阵的一些基本特征．     

多普勒径向速度图中零等速线应用初探

指出了零等速线在阿克苏地区多普勒雷达的径向速度图分析中的重要作用,并对零等速线进行了说明、分析,为多普勒径向速度图的分析提供一些依据.     

防雷工程中的电源避雷器与零地合一问题浅析

在信息系统综合防雷工程设计施工过程中,为解决电源各输电线路之间因电流不相等而产生的用户端零线对地的电位差,即零地电压对设备的危害,以及防止设备因供电断零线而损坏的情况,需要对零线重复接地,把零地电压控制在一定的范围之内（雷达机房要求〈2V）。通过分析一起按规范安装电源避雷器与零地处理引起的事故,提出防雷工程整改完善的建议,为同类工作提供参考依据。     

高空气象探测的静态特征量

根据高空气象探测系统的业务需求,较为详细地介绍了灵敏度、量程及测量范围、线性度、迟滞、重复性、准确度、分辨率、漂移等探测系统的静态特征量。     

菲律宾皮纳图博火山爆发的卫星探测分析

应用气象卫星的探测处理资料，揭示和探讨了1991年6月15日菲律宾皮纳图博火山爆发后火山灰和火山尘云的演变和漂移中的一些重要特征，为研究这次火山爆发对天气和气候的影响提供了卫星观测分析信息。     

高空气象探测的静态特征量

根据高空气象探测系统的业务需求,较为详细地介绍了灵敏度、量程及测量范围、线性度、迟滞、重复性、准确度、分辨率、漂移等探测系统的静态特征量.     

A note on ‘separation’ over short wind waves

Whether or not separation occurs in the airflow over wind-generated water waves is partly a question of semantics but also has an important bearing on the wave generation process. In the present paper we use a rather formal and perhaps narrow definition of separation and show that it does not occur where the shear stress is zero but only in conjunction with wave breaking. This is unlikely to happen except in the presence of quite strong surface drift velocities in the water. A similar connection between separation, surface drift and wave breaking has recently been established by Banner and Melville (1976).The effects of increasing wave amplitude or steepness are investigated with a numerical model of the airflow over water waves. Variations in the depth of the closed streamline region are predicted. The model is also used to investigate the possible importance of surface drift velocities.On leave 1976, Atmospheric Environment Service, Downsview, Ont., Canada.     

Revision and necessary correction of the long-term temperature series of Hohenpeissenberg, 1781–2006

Having been in use at Hohenpeissenberg from 1781–1841, the Palatina thermometer was found to suffer from a positive bias of 0.5°R (or 0.63°C) as discovered by Lamont following a re-calibration made in 1842. The main reason was due to the composition of the glass used during the early instrumental period. Glass of this period tended to contract over many years due to thermal aftereffects, resulting in a gradual rise of the freezing point position in consequence of the shrinking bulb forming the mercury reservoir. While the problem of the gradually rising zero point was recognised relatively early, the reason was attributed to wrong causes. Around 1880, scientists recognised that the chemical composition of glass might be responsible for the drift of the zero point. New glass types were developed which were free from such effects. Although these facts became known, no correction was applied to the Hohenpeissenberg temperature series when in 1981, the complete 200-year series was published. Most probably this bias is also relevant for other stations, at least those of the network of the Societas Meteorologica Palatina that were supplied with thermometers manufactured in Mannheim. Another problem originates from the different observing times for the period 1879–1900, which were set to 0800, 1400 and 2000 hours instead of 0700, 1400 and 2100 hours before and afterwards. In addition, a new formula to calculate the daily mean was established resulting in the temperature being too low by 0.5°C in that period. The overall trend changes after application of the two necessary corrections. There remain two biases that cannot be quantified without a major detailed study being made: (1) At the start of the observations, the window of the observation room was always kept “open during dry weather”. It is not known how long this practice was remained in use. (2) Lamont also employed an easily melting glass to construct his thermometers which in use between 1841 and 1878. An analysis of the glass composition seems to be necessary to find out whether it also suffered from a rising freezing point. Lamont replaced the Hohenpeissenberg thermometer in 1842 by a new instrument produced in his own workshop. One still existing Lamont thermometer, but not that one of Hohenpeissenberg, was re-calibrated and the zero point found to have lowered by ?1.4°C. Since the opposite drift had been expected and the original Lamont-type Hohenpeissenberg thermometer is no longer available, no correction is justified for the period in which this thermometer was in use.     

The effects of precipitation and river runoff in a coupled ice-ocean model of the Arctic

A coupled ice-ocean model of the Arctic is developed in order to study the effects of precipitation and river runoff on sea ice. A dynamic-thermodynamic sea ice model is coupled to an ocean general circulation model which includes a turbulent closure scheme for vertical mixing. The model is forced by interannually varying atmospheric temperature and pressure data from 1980–1989, and spatially varying mean monthly precipitation and river runoffs. Salinity and fresh water fluxes to the ocean from ice growth, snow melt, rain, and runoffs are computed, with no artificial constraints on the ocean salinity. The modeled ice thickness is similar to the observed pattern, with the thickest ice remaining against the Canadian Archipelago throughout the year. The modeled ice drift reproduces the Beaufort gyre and Transpolar drift exiting through Fram Strait. The stable arctic halocline produced by the vertical mixing scheme isolates the surface from the Atlantic layer and reduces the vertical fluxes of heat and salinity. A sensitivity experiment with zero precipitation results in rapidly decreasing ice thickness, in response to greater ocean heat flux from a weakening of the halocline, while an experiment with doubled precipitation results in a smaller increase in ice thickness. A zero-runoff experiment results in a slower decrease in ice thickness than the zero-precipitation case, due to the decadal time scale of the transport of runoff in the model. The results suggest that decadal trends in both arctic precipitation and river runoffs, caused either by anthropogenic or natural climatic change, have the potential to exert broad-scale impacts on the arctic sea ice regime. Received: 6 February 1996 / Accepted: 4 April 1996     

GPS掩星切点水平漂移规律的数值研究

在现有GPS星座和大气球对称假设条件下，利用射线追踪法对掩星事件进行了数值模拟，讨论了大气折射指数垂直分布、LEO卫星轨道倾角和高度对GPS掩星切点水平漂移的影响情况。结果表明:在太阳活动剧烈的白天和夜间两种典型情况下，切点平均水平漂移变化约20 km；对735 km高度的LEO卫星来说，轨道倾角在130°附近时，切点平均水平漂移最小，并随着倾角向0°或180°变化，切点平均水平漂移均增大，但在55°附近时随倾角变化稍有波动；对倾角为70°的LEO卫星来说，当轨道高度从400 km变化到1500 km时，切点平均水平漂移变化约141 km，且随高度增加而单调减小     

The ACPI Project, Element 1: Initializing a Coupled Climate Model from Observed Conditions

A problem for climate change studies with coupled ocean-atmosphere models has been how to incorporate observed initial conditions into the ocean, which holds most of the `memory' of anthropogenic forcing effects. The first difficulty is the lack of comprehensive three-dimensional observations of the current ocean temperature (T) and salinity (S) fields to initialize to. The second problem is that directly imposing observed T and S fields into the model results in rapid drift back to the model climatology, with the corresponding loss of the observed information. Anthropogenic forcing scenarios therefore typically initialize future runs by starting with pre-industrial conditions. However, if the future climate depends on the details of the present climate, then initializing the model to observations may provide more accurate forecasts. Also, this ～ 130 yr spin up imposes substantial overhead if only a few decades of predictions are desired. A new technique to address these problems is presented. In lieu of observed T and S, assimilated ocean data were used. To reduce model drift, an anomaly coupling scheme was devised. This consists of letting the model's climatological (pre-industrial) oceanic and atmospheric heat contents and transports balance each other, while adding on the (much smaller) changes in heat content since the pre-industrial era as anomalies. The result is model drift of no more than 0.2 K over 50 years, significantly smaller than the forced response of 1.0 K. An ensemble of runs with these assimilated initial conditions is then compared to a set spun up from pre-industrial conditions. No systematic differences were found, i.e., the model simulation of the ocean temperature structure in the late 1990s is statistically indistinguishable from the assimilated observations. However, a model with a worse representation of the late 20th century climate might show significant differences if initialized in this way.     

Modeling Iceberg Drift in the Barents Sea from Field Data

The iceberg drift model is developed and used for simulating the iceberg drift trajectory in the Barents Sea. The model is forced by hydrometeorological characteristics obtained from ship observations. Original techniques for retrieving the sea-level slope gradient and surface velocity of currents are proposed, implemented, and validated using independent data. Thus, additional data were calculated from field data in order to use the iceberg drift model with the full set of external forces. This allowed improving the iceberg trajectory simulation and assessing the contribution of all forces that affect the iceberg drift. The iceberg drift calculations demonstrate that the drift characteristics are extremely sensitive to all external effects and the model parameters; therefore, the quality of input hydrometeorological data essentially affects the simulation of real iceberg trajectories.     

Evaluation of Arctic Sea Ice Drift and its Relationship with Near-surface Wind and Ocean Current in Nine CMIP6 Models from China

The simulated Arctic sea ice drift and its relationship with the near-surface wind and surface ocean current during 1979-2014 in nine models from China that participated in the sixth phase of the Coupled Model Intercomparison Project(CMIP6)are examined by comparison with observational and reanalysis datasets.Most of the models reasonably represent the Beaufort Gyre(BG)and Transpolar Drift Stream(TDS)in the spatial patterns of their long-term mean sea ice drift,while the detailed location,extent,and strength of the BG and TDS vary among the models.About two-thirds of the models agree with the observation/reanalysis in the sense that the sea ice drift pattern is consistent with the near-surface wind pattern.About the same proportion of models shows that the sea ice drift pattern is consistent with the surface ocean current pattern.In the observation/reanalysis,however,the sea ice drift pattern does not match well with the surface ocean current pattern.All nine models missed the observational widespread sea ice drift speed acceleration across the Arctic.For the Arctic basin-wide spatial average,five of the nine models overestimate the Arctic long-term(1979-2014)mean sea ice drift speed in all months.Only FGOALS-g3 captures a significant sea ice drift speed increase from 1979 to 2014 both in spring and autumn.The increases are weaker than those in the observation.This evaluation helps assess the performance of the Arctic sea ice drift simulations in these CMIP6 models from China.     

TOGA型海-气耦合模式直接模拟的SST误差分析

本文对一个TOGA(热带太平洋和全球大气)型耦合环流模式直接耦合30 a(1980—2009年)的模拟结果进行分析,发现模拟的热带太平洋海表温度存在严重的"气候漂移"现象。通过对模式海表温度控制方程中加热和冷却项的分析,特别是对海表热通量和风应力的分析,指出了两者的误差在热带太平洋海表温度的"气候漂移"现象中扮演的角色。为了进一步证实分析的结果,通过4个敏感性试验分析热通量和风应力对热带太平洋海表温度分布的作用,特别是热通量对西太平洋暖池的形成,而风应力对东太平洋冷舌的形成均有重要的作用以及纬向风应力和经向风应力对冷舌形成的相对贡献。     

Comparison of Canadian daily ice charts with surface observations off Newfoundland,winter 1992

Abstract

Forecast ice drift rates and thicknesses displayed on daily ice charts and forecast winds for the Canadian east coast are compared to on‐ice observations made during the second Canadian Atlantic Storm Program (CASP II) of March 1992. Observed and 24‐hour forecasts of daily ice drift rates were weakly correlated even though long‐term means closely matched observations. Daily drift rates have an RMS error of 13 cm s^‐1 relative to a 15 cm s^‐1 mean in addition to an RMS direction error of 50 degrees. Contributions towards daily drift uncertainties were: the estimation of winds, unmodelled physics of ocean and ice cover processes; and the inconsistency in the methods used by the ice forecaster. Correlation coefficients between forecast winds and on‐ice observed winds decreased from 0.8 at 0‐hour to 0.7 for the 30‐hour forecast. Similar results were found between ice drift rates from forecast winds. Histograms of ice thicknesses observed along narrow swaths using a helicopter‐towed electromagnetic sensor compared well with undeformed ice thicknesses representing large areas on ice charts, with differences mainly caused by difference in ice type representation and by co‐registering the two data sets.