基于海气通量算法的海上蒸发波导诊断模型

蒸发波导是海上普遍存在的海洋天气现象, 也是导致海上电磁波异常传播的重要因素, 严重影响了海上雷达、通信及电子设备的有效应用。而TOGA COARE (海洋-大气耦合响应试验) 通量算法为蒸发波导的精确诊断提供了条件, 因此, 该文建立了基于海气通量算法的海上蒸发波导诊断模型, 并利用福建海域铁塔观测资料以及海上雷达探测试验数据与美国业务运转的Paulus-Jeske诊断模型对比, 结果表明:通量蒸发波导诊断模型的各项对比结果均优于Paulus-Jeske模型。     

4种蒸发波导模型的对比与分析

蒸发波导模型常用来计算海上蒸发波导高度。为了认识当前不同蒸发波导模型之间的差异和方法,本文选取了目前使用广泛的4种蒸发波导模型(即P-J模型、Babin模型、NPS模型和伪折射率模型)进行对比和分析。本文首先探讨了在理想情况下它们对气象要素的敏感性,随后并利用我国南海近海大气层观测试验数据对比了这4种模型的蒸发波导高度计算结果。分析表明:相对湿度、风速和气—海温差的变化对4种模型的计算都有着较大的影响,特别是在不稳定层结状况下,4种模型计算得到的蒸发波导高度都随着相对湿度的增大而降低、随着风速的增大而增高。Babin模型和NPS模型计算的波导高度较为一致,伪折射率模型与前两种模型的计算结果存在差异,而P-J模型与其他3种模型存在较明显的偏差。基于南海气象数据的计算结果表明,不同蒸发波导模型在该海域蒸发波导的模拟结果略有不同,但4种模型计算得到的波导高度日变化变化趋势较为一致,波导高度极低值常出现在早晨,而极高值常出现在傍晚。     

用于风电场功率预测的逐时风速预报

为满足风电场精细化风速预报的需要,利用MM5模式的格点输出数值预报产品以及福建沿海地区两座海上测风塔的逐时气象资料,采用逐步回归的统计方法,将MM5数值预报产品与测风塔实测气象资料要素指标值共同引入回归方程,拟合两座测风塔特定高度的逐小时风速预报方程,详细介绍了该方法的实现过程.通过一年的预报效果指标以及15日的独立样本效果检验,结果表明该方法对于逐小时风速的预报有一定的应用价值.     

大气波导特征分析及其对电磁波传播的影响

文中在介绍大气折射的基本类型及其存在条件的基础上 ,阐述了三种类型的大气波导的形成机制 ,总结并分析了大气波导的几个主要特征 ,并用西北太平洋云辐射实验的实测资料和西沙海域的气象资料进行了验证 ,同时试验了蒸发波导高度对大气湿度、气海温差、水平风速变化的敏感性 .在分析大气波导对电磁波传播的影响时 ,推导了可形成波导传播的电磁波最大陷获波长和临界发射仰角 ,提出了电磁波形成波导传播的 4个必要条件 ,并讨论了大气波导对超短波传播、雷达探测、短波通信等方面的影响 .     

一次黑潮海洋锋强迫下的蒸发波导突变性与非均匀性的观测与模拟研究

蒸发波导是影响海上雷达系统探测性能的主导机制,海表温度（SST）锋带来的蒸发波导非均匀性和突变性具有重要的研究价值。2018年春季航次“海气相互作用观测试验”,曾两次穿越黑潮海域获取了珍贵的观测资料。在此基础上,结合欧洲中期天气预报中心（ECMWF）再分析资料（ERA-Interim）和HYSPLIT（Hybrid Single Particle Lagrangian Integrated Trajectories）气块轨迹溯源,分离出两个重要的走航观测时段。S1段（持续约21 h）气流从暖海水区吹向冷海水区,以稳定层结为主,其间因黑潮海洋锋的存在,气流由黑潮主体的暖水区吹向大陆冷海区时,形成具有强逆温层的海洋边界层,并伴随海雾的生成,导致此处蒸发波导高度突降为0。此后为持续近66 h的S2段,气流由冷海水区吹向暖海水区,以近中性弱不稳定层结为主,蒸发波导高度基本维持在12 m高度。数值模拟结果表明,模拟时段内的黑潮海洋锋区,蒸发波导高度突变性和非均匀性始终存在,且伴随暖海水吹向冷海水的锋区突变性更强。黑潮海洋锋对蒸发波导的这种天气尺度强迫作用的加强与层结稳定度的突变和海雾的生成有关。      

1998年季风试验期间南海蒸发波导特征分析

利用1998年南海季风试验期间“科学1号”和“实验3号”科考船每天四次的高分辨率探空数据,分析了南海季风爆发前后蒸发波导特征。结果表明:南海季风爆发后蒸发波导发生概率大于爆发前,且南海南部发生概率大于北部;南海蒸发波导具有明显的日变化特征,总体上呈现“低-高-低”的趋势,波导强度日变化比波导高度日变化剧烈;季风爆发前的波导强度和高度比爆发后的方差小,较稳定;季风期间南海南部的波导强度总体上比北部强,波导高度比北部低。这可能是西南季风的爆发改变了近海面大气边界层结构引起的。      

"神舟六号"飞船着陆时段主着陆场区风场的数值模拟

本文通过分析"神舟六号"飞船着陆时期WRF模式对主着陆场区的风场及其影响系统的模拟结果, 发现WRF模式对主着陆场区的地面风速、风向的预报,WRF模式输出的850 hPa 模拟风场对100 m高度以下浅层风的最大风速及其风向的预报,结果均比较理想;WRF模式输出的300 hPa 高度风速、风向的模拟结果和急流轴的强度、位置模拟结果,与高空7～12 km最大风速及其风向的相关性较好,可作为预报指标;模式对风场的主要影响系统东北低压加深东移和蒙古高压的演变模拟基本准确.本模式能够作为未来客观预报主着陆场区地面和高空风场一种新的技术手段和工具.     

大气波导形成条件及传播路径模拟

推导了可形成波导传播的电磁波最大陷获波长和临界发射仰角,介绍了电磁波可形成波导传播的必要条件,在此基础上建立了在大气波导层中电磁波传播路径模式,并利用南京雷达实际观测的超折射回波对此模式进行了验证,所得结果比较一致。     

2019—2020年非汛期Grapes_1km 10m风速预报检验评估

选取广东省53个国家基本站,对2019年10月—2020年3月Grapes_1 km模式输出的10 m风场进行检验,发现Grapes_1 km预报与实况整体趋势较一致,但预报10 m风极大值的峰值略有提前;相关性检验方面,相关性比较好的地区是湛江沿海地区、江门沿海、汕头沿海,相关性较差的地区分别是茂名沿海、云浮地区、汕尾沿海;预报命中率随着风速的加大呈明显下降的趋势,且沿海站点的命中率略好于内陆站点;随着风速的增大,预报值相对实况有偏小的趋势。     

风廓线雷达与多普勒天气雷达风矢产品对比及相关分析

利用成都地区2010年8月和北京沙河地区2011年7—8月风廓线雷达以及多普勒天气雷达的风廓线探测资料,结合对应时段的天气现象相关记录,通过对比分析得到以下结论:①弱降水条件下,在300~2100m高度内,风廓线雷达与多普勒天气雷达探测具有很好的相关性,风向相关系数平均值为0.596,风速相关系数平均值为0.736,在做预报时两者可以同时应用,互为补充;②强降水天气条件下,风廓线雷达与多普勒天气雷达探测的风向、风速变化趋势基本一致,特别是在300~2100m之间各个高度上风向、风速相关性较好,风向相关系数平均值为0.573,风速相关系数为0.508,且风廓线雷达比多普勒天气雷达探测到的各层风向、风速变化更为详细、直观;③阴天条件下风廓线雷达与多普勒天气雷达的风向、风速相关性低层比高层好;④晴天条件下,风廓线雷达更适合用于预报和监测天气。     

滨州沿海蒸发量与海盐产量的关系研究

海盐生产主要依靠自然蒸发,蒸发量预报对海盐生产有重要的指导作用。通过对1993—2007年滨州沿海蒸发量和海盐产量的分析,海盐产量的时间分布特征与净蒸发量基本一致,净蒸发量是影响海盐生产的决定性因素。分析蒸发量与气象要素之间的关系,分月建立了逐步回归方程,经检验可作为蒸发量的一种客观预报方法。     

ANALYSIS ON CHARACTERISTICS OF ATMOSPHERIC DUCT AND ITS EFFECTS ON THE PROPAGATION OF ELECTROMAGNETIC WAVE

On the basis of introducing the basic categories of atmospheric refraction and their existingconditions,the forming processes of three kinds of atmospheric ducts are expounded.Several maincharacteristics of atmospheric duct are summarized and analyzed,and field sounding data from theWEstern North-Pacific cloud-radiation EXperiment(WENPEX)and meteorological data aroundthe Xisha sea area are used to validate these characteristics.Meanwhile the sensitivities of theevaporation duct height to the variations of atmospheric humidity.the air-sea temperaturedifference.and horizontal wind speed are examined.With the analysis of the effect of atmosphericduct on the propagation of electromagnetic wave.the maximum trapped-wavelength and the criticalemitting angle of elevation for electromagnetic wave which can form duct propagation are derived.At the same time the four kinds of necessary conditions for electromagnetic wave to form ductpropagation are brought forward.The effects of atmospheric duct on ultrashort wave propagation,radar observation.short wave communication etc.are also discussed.     

ANALYSIS ON CHARACTERISTICS OF ATMOSPHERIC DUCT AND ITS EFFECTS ON THE PROPAGATION OF ELECTROMAGNETIC WAVE*

On the basis of introducing the basic categories of atmospheric refraction and their existing conditions,the forming processes of three kinds of atmospheric ducts are expounded.Several main characteristics of atmospheric duct are summarized and analyzed,and field sounding data from the WEstern North-Pacific cloud-radiation EXperiment(WENPEX) and meteorological data around the Xisha sea area are used to validate these characteristics.Meanwhile the sensitivities of the evaporation duct height to the variations of atmospheric humidity.the air-sea temperature difference.and horizontal wind speed are examined.With the analysis of the effect of atmosphericduct on the propagation of electromagnetic wave.the maximum trapped-wavelength and the critical emitting angle of elevation for electromagnetic wave which can form duct propagation are derived.At the same time the four kinds of necessary conditions for electromagnetic wave to form ductpropagation are brought forward.The effects of atmospheric duct on ultrashort wave propagation,radar observation.short wave communication etc.are also discussed.     

Numerical Study on the Impacts of the Bogus Data Assimilation and Sea Spray Parameterization on Typhoon Ducts

The Weather Research and Forecasting model version 3.2 (WRF v3.2) was used with the bogus data assimilation (BDA) scheme and sea spray parameterization (SSP), and experiments were conducted to assess the impacts of the BDA and SSP on prediction of the typhoon ducting process induced by Typhoon Mindule (2004). The global positioning system (GPS) dropsonde observations were used for comparison. The results show that typhoon ducts are likely to form in every direction around the typhoon center, with the main type of ducts being elevated duct. With the BDA scheme included in the model initialization, the model has a better performance in predicting the existence, distribution, and strength of typhoon ducts. This improvement is attributed to the positive effect of the BDA scheme on the typhoon’s ambient boundary layer structure. Sea spray affects typhoon ducts mainly by changing the latent heat (LH) flux at the air-sea interface beyond 270 km from the typhoon center. The strength of the typhoon duct is enhanced when the boundary layer under this duct is cooled and moistened by the sea spray; otherwise, the typhoon duct is weakened. The sea spray induced changes in the air-sea sensible heat (SH) flux and LH flux are concentrated in the maximum wind speed area near the typhoon center, and the changes are significantly weakened with the increase of the radial range.     

台风外围下沉区大气波导成因的数值模拟

受台风鹿莎影响,处在其西侧外围下沉区域的南京地区于2002年8月31日出现了一次大气波导过程,利用大气中尺度模式WRF对其成因进行了详细的数值模拟研究。WRF数值模拟较好地再现了此次波导的演变过程,即波导在31日傍晚开始形成,次日凌晨达到最强,日出后迅速减弱消失。基于数值模拟高时空分辨率的输出结果,对波导成因进行细致分析,结果表明:湿度突变层和逆温层的同时存在导致了波导的发生,前者是其形成的关键因素,而后者的作用主要体现在增强其强度;台风前期流场从海上带来大量的水汽,台风后期流场将北方高空干空气输送到受高压下沉运动控制的南京地区,造成近地层出现下湿上干的剧烈湿度梯度;下沉运动强度并不足以直接导致南京地区的逆温层,但其控制下的晴朗天气非常有利于夜间地面长波辐射冷却而形成逆温。     

Precipitation and evaporation budgets over the Baltic Proper: observations and modelling

Precipitation and evaporation budgets over the Baltic Sea were studied in a concerted project called PEP in BALTEX (Pilot study of Evaporation and Precipitation in the Baltic Sea), combining extensive field measurements and modelling efforts. Eddy-correlation-measurements of turbulent heat flux were made on a semi-continuous basis for a 12 month period at four well-exposed coastal sites in the Baltic Proper (the main basin of the Baltic Sea). Precipitation was measured at land-based sites with standard gauges and on four merchant ships travelling between Germany and Finland with the aid of specially designed ship rain gauges (SRGs). The evaporation and precipitation regime of the Baltic Sea was modelled for a 12 month period by applying a wide range of numerical models: the operational atmospheric High Resolution Limited Area Model (HIRLAM, Swedish and Finnish versions), the German atmospheric REgional-scale MOdel, REMO, the operational German Europe Model (only precipitation), the oceanographic model PROBE-Baltic, and two models that use interpolation of ground-based data, the Swedish MESAN model of SMHI and a German model of IFM-GEOMAR Kiel. Modelled precipitation was compared with SRG measurements on board the ships. A reasonable correlation was obtained, but the regional-scale models and MESAN gave some 20% higher precipitation over the sea than is measured. Bulk parameterisation schemes for evaporation were evaluated against measurements. A constant value of C_HN and C_EN with wind speed, underestimated large fluxes of both sensible and latent heat flux. The limited area models do not resolve the influence of the height of the marine boundary layer in coastal zones and the entrainment (on the surface fluxes), which may explain the observed low correlations between modelled and measured latent heat fluxes. Estimates of evaporation, E, and precipitation, P, for the entire Baltic Proper were made with several models for a 12 month period. While the annual variation was well represented by all predictions, there are still important differences in the annual means. Evaporation ranges from 509 to 625 mm year^-1 and precipitation between 624 and 805 mm year^-1 for this particular 12 month period. Taking the results of model verification from the present study into account, the best estimate of P-E is about 100 ± 50 mm for this particular 12 month period. But the annual mean of P-E varies considerably from year to year. This is reflected in simulations with the PROBE-Baltic model for an 18 year period, which gave 95 mm year^-1 for the 12 month period studied here and 32 mm year^-1 as an average for 18 years.