辐射方案对GRAPES全球模式的影响

辐射过程是中期数值天气预报模式和气候模式中一个重要的物理过程。本文针对GRAPES (Global/Regional Assimilation and PrEdiction System) 全球模式非静力半隐式半拉格朗日的特点, 进行了不同辐射方案的敏感性比较试验, 以期找到一个适合于GRAPES全球模式的辐射方案。用到的方案包括WRF模式中的RRTM长波辐射方案、 NASA的Goddard短波辐射方案以及ECMWF的长短波辐射方案。试验结果表明, ECMWF的辐射方案更适合于GRAPES模式, 30天平均的北半球500 hPa高度场距平相关系数较WRF的辐射方案提高了近2%。另外, 针对实际运行中存在的辐射计算不稳定问题, 对辐射方案进行了气压订正和温度订正, 并对2005年7月影响我国的海棠台风进行了模拟试验, 气压订正后的120小时模式预报在对副热带高压和台风的描述上更接近于分析, 可用预报时效也有了明显提高。     

辐射传输模式中地表参数对大气长波辐射的影响

本文利用Liou-Ou一维宽带辐射传输模式，对地表热力参数取值部分作了改进，使用模式大气和青藏高原实测资料对下垫面温度与地表空气温度两者不能合二为一的问题进行了分析，同时还讨论了下垫面温度的日变化对大气长波辐射通量日变化的影响及地表比辐射率的变化对大气长波辐射通量计算结果的修正作用。     

烟雾层的长波辐射效应以及对边界层温度层结的影响

本文利用一个简化的长波辐射方案，计算了兰州城市烟雾层大气的辐射效应．计算表明:烟雾层气溶胶增加了到达地面的大气逆辐射和气层的冷却率，平均污染状况时，增加量分别为15．2％和0．073℃／h．与烟雾层对太阳辐射吸收加热率相比，冷却率量值较小，但对全天边界层能量平衡所起作用不可忽略．对比分析了兰州和郊区夜晚的平均温度廓线演变情况，可以看出烟雾层长波辐射效应增加了低层大气中上部的冷却．     

ECMWF业务预报系统的改进

欧洲中期预报中心(ECMWF)第二个业务模式——T63(谱模式)1983年4月21日投入业务使用后,进行了以下改进:1984年12月4日,改进了辐射格式,在解决长波辐射传输方面,使用了与过去不同的气体效应处理方法,其最大好处是缓和了中、高对流层中,云量少的层次所出现的过     

成都东北部地区太阳辐射特征分析

该文利用2018年1月—12月成都东北部地区的太阳辐射观测资料,分析了辐射能量的收支状况和特征。结果表明:成都东北部地区各辐射分量(除净长波辐射)均是夏季最强,冬季最弱,最大值出现在8月。净长波辐射春季最强,秋季最弱,与空气相对湿度、气温日较差分别成负相关、正相关。净全辐射白天为正值,晚上为负值。成都东北部地区全年有10.7%的太阳短波辐射被地表反射,接收的太阳短波辐射有29.36%被地表以长波辐射的方式释放到大气,对地气系统能量收支的贡献为61.18%。     

利用MODIS-GOCART气溶胶资料研究中国东部地区气溶胶直接辐射强迫

利用MODIS-GOCART同化的2001年逐月气溶胶光学厚度资料，在修改区域气候模式RegCM2辐射方案的基础上，连续积分5年获得平均的中国东部地区气溶胶短波和长波直接辐射效应，并通过数值试验研究了气溶胶垂直分布对辐射强迫及其气候响应的影响。结果表明：气溶胶的短波辐射效应能冷却地表、加热大气；长波辐射效应能加热地表、冷却大气；大气顶净辐射强迫年平均为-4．1W／m^2；辐射强迫绝对值在春季最大，夏季次之，冬季最小；模拟区域中最大辐射强迫值主要位于华北、华南地区及四川盆地；气溶胶垂直分布是影响气溶胶辐射强迫的重要因素。总体上气溶胶层越靠近地面，大气顶辐射强迫绝对值越大，地表辐射强迫绝对值越小，大气顶辐射强迫对垂直分布较敏感；气候系统的反馈作用会放大气溶胶垂直分布对辐射气候效应的影响。     

塔克拉玛干沙漠腹地的长波辐射变化特征

利用塔克拉玛干沙漠大气环境观测试验站(塔中站)实测的长波辐射资料,分析了流动沙漠区的长波辐射特征.结果表明:地表长波辐射能具体地反映地表失去热能的状况.在沙漠区,由于地表层的湍流运动较强以及下垫面温度与空气温度的差值较大,使得地表向大气传输的热通量较大,所以地面长波辐射值较大,有时接近于总辐射,最小值出现在日出前,最大值出现在15:00左右;由于大气中的水汽含量及云量较少,而沙尘气溶胶含量较高,所以大气长波辐射较大,沙漠区有效辐射也较大,为我国有效辐射年总量最高的地区之一.地表放射的净长波辐射在太阳总辐射中所占的比例小于地表反射辐射,只有在春、夏季两者较接近,且以反射辐射大些.区域气候变化过程中,沙漠加热场的强度是沙漠局地天气气候变化的主要影响因素之一.     

从FY-4A卫星遥感数据和GFS资料估算全天空状况下的地表长波辐射通量

本文介绍一种利用FY-4A成像仪遥感数据和全球预报系统(GFS)资料估算全天空地表长波辐射通量的反演方法。该方法通过辐射传输模拟和统计回归计算建立云天地表下行长波辐射通量的反演模式,并基于GFS资料处理云覆盖地区的地表上、下行长波辐射通量。这种全天空状况下两种通量的反演结合了FY-4A晴空地表长波辐射业务产品和本文反演模式处理的云天地表上、下行长波辐射通量。2018年9月1日的处理结果与Aqua/CERES同类产品相对比,精度为:RMSE=20.52 W·m^-2,R=0.9481,Bias=3.3 W·m^-2(夜间地表下行辐射通量对比);RMSE=25.58 W·m^-2,R=0.9096,Bias=5.4 W·m^-2(白天地表下行辐射通量对比);RMSE=10.97 W·m^-2,R=0.9762,Bias=-3.3 W·m^-2(夜间地表上行辐射通量对比);RMSE=19.97 W·m^-2,R=0.9283,Bias=5.0 W·m^-2(白天地表上行辐射通量对比)。这些结果表明本文发展的方法能够反演出精度较好的云天上下行长波辐射通量资料,为今后利用FY-4后续星处理生成全天空状况下的地表长波辐射通量产品奠定了理论基础。     

长波辐射对大气变化的敏感性和在WRF模式中的应用检验

用RRTM长波辐射 (LWR)参数化方案测试了LWR对大气变化的敏感性。结果表明 :高云对向外长波辐射(OLR)、30 0和 5 0 0hPa净LWR通量的减弱作用较中、低云大 ;低云对 85 0hPa和地表净LWR通量的减弱作用较中、高云大。在云层中 ,LWR冷却率受云影响最大 ;在云层下方 ,云对LWR的影响迅速减小 ;而在云层上方 ,冷却率几乎不受云的影响。当水汽含量减少或增加时 ,地表向下LWR受到相应减弱或增强 ,而净LWR则在一定程度上受到相应增强或减弱 ,并且越接近地面 ,受到水汽变化的影响就越大。O3 对LWR的影响相对云和水汽来说是比较小的。文中介绍了在WRF模式中应用RRTM方案预报LWR不同季节的 2个个例 ,给出了应用NCEP/AVN分析资料预报和验证中国范围 2d之内LWR通量的模拟结果。试验表明 ,OLR和 5 0 0hPa净LWR通量与高度形势场有较好的对应关系 ,而地表净LWR很大程度上还受到地形的影响。     

Precipitation responses to radiative processes of water- and ice-clouds: an equilibrium cloud-resolving modeling study

云辐射过程对制约天气与气候很重要。本文通过分析二维云分辨模式敏感性试验模拟平衡态平均资料研究降水对水云及冰云辐射过程的响应。模式给定的垂直速度为零。存在冰云辐射过程时去除水云辐射过程,以及去除冰云辐射过程会加强大气长波辐射冷却和降低空气温度及饱和混合比。饱和混合比的减少导致水汽凝结增加及其相关的潜热释放的增加,从而增加降雨。去除水云辐射过程通过减少长波辐射冷却增加对流层上部局地大气变暖。而增强的变暖通过霰的融化增强而增加降水源与降水。     

A one-dimensional simulation of the stratocumulus-capped mixed layer

A marine stratocumulus model has been developed which has four major sub-models: (1) a one-dimensional version of the CSU cumulus model, (2) a partially-diagnostic higher-order turbulence model, (3) an atmospheric radiation model for both short-wave and long-wave radiation, and (4) a partial condensation scheme and cloud fractional parameterization. A set of numerical experiments have been performed to study the interactions among the turbulence, the long-wave radiation, the short-wave radiation, and the sub-grid condensation processes. The results indicate that surface sensible eddy heat flux and not radiative cooling is the major control on the rate of cloud-top entrainment. Cloud-top radiation cooling occurs principally within the upper part of the mixed layer. However, for the stratocumulus with numerous towers penetrated into the capping inversion, most of the long-wave radiation occurs within the capping inversion. It is found that cloud-top radiation cooling is balanced by turbulence transport of sensible heat from cloud-base levels.     

Direct measurements of radiative and turbulent flux convergences in the lowest 1000 m of the convective boundary layer

Results derived from simultaneous measurements of turbulent heat flux and radiation convergence in the daytime convective boundary layer are presented. It is found that the effects of long-wave radiation result in a warming near the surface and cooling at higher levels, in good agreement with infra-red radiative transfer models. Heating rates, roughly 30% of those produced by turbulence, are observed as a result of the absorption of short-wave radiation in the lowest 1000 m of the atmosphere.     

The radiation budget in a regional climate model

The long- and short-wave components of the radiation budget are among the most important quantities in climate modelling. In this study, we evaluated the radiation budget at the earth??s surface and at the top of atmosphere over Europe as simulated by the regional climate model CLM. This was done by comparisons with radiation budgets as computed by the GEWEX/SRB satellite-based product and as realised in the ECMWF re-analysis ERA40. Our comparisons show that CLM has a tendency to underestimate solar radiation at the surface and the energy loss by thermal emission. We found a clear statistical dependence of radiation budget imprecision on cloud cover and surface albedo uncertainties in the solar spectrum. In contrast to cloud fraction errors, surface temperature errors have a minor impact on radiation budget uncertainties in the long-wave spectrum. We also evaluated the impact of the number of atmospheric layers used in CLM simulations. CLM simulations with 32 layers perform better than do those with 20 layers in terms of the surface radiation budget components but not in terms of the outgoing long-wave radiation and of radiation divergence. Application of the evaluation approach to similar simulations with two additional regional climate models confirmed the results and showed the usefulness of the approach.     

利用简单生物圈模式SiB2模拟锡林浩特草原地表湍流通量

利用简单生物圈模式SiB2模拟了2007年7月1日至9月30日期间锡林浩特草原的地表能量分配、CO2通量、地表有效辐射温度和土壤湿度.采用锡林浩特国家气候观象台野外试验基地实地测量资料确定SiB2所需要的参数和初始值后,由该资料中30 min一次的太阳短波辐射、大气长波辐射、水汽压、气温、水平风速和降水驱动SiB2,最...     

青藏高原地区OLR与地面有效辐射关系的分析

青藏高原;;OLR;;地面有效辐射     

The surface radiation budget over South America in a set of regional climate models from the CLARIS-LPB project

The performance of seven regional climate models in simulating the radiation and heat fluxes at the surface over South America (SA) is evaluated. Sources of uncertainty and errors are identified. All simulations have been performed in the context of the CLARIS-LPB Project for the period 1990–2008 and are compared with the GEWEX-SRB, CRU, and GLDAS2 dataset and NCEP-NOAA reanalysis. Results showed that most of the models overestimate the net surface short-wave radiation over tropical SA and La Plata Basin and underestimate it over oceanic regions. Errors in the short-wave radiation are mainly associated with uncertainties in the representation of surface albedo and cloud fraction. For the net surface long-wave radiation, model biases are diverse. However, the ensemble mean showed a good agreement with the GEWEX-SRB dataset due to the compensation of individual model biases. Errors in the net surface long-wave radiation can be explained, in a large proportion, by errors in cloud fraction. For some particular models, errors in temperature also contribute to errors in the net long-wave radiation. Analysis of the annual cycle of each component of the energy budget indicates that the RCMs reproduce generally well the main characteristics of the short- and long-wave radiations in terms of timing and amplitude. However, a large spread among models over tropical SA is apparent. The annual cycle of the sensible heat flux showed a strong overestimation in comparison with the reanalysis and GLDAS2 dataset. For the latent heat flux, strong differences between the reanalysis and GLDAS2 are calculated particularly over tropical SA.     

层状云微物理参数反演及其辐射效应的个例研究

利用毫米波云雷达、微波辐射计联合反演方法,对2015年11月11日安徽寿县的一次层状云过程的云参数进行了反演,将所得云参数加入到SBDART辐射传输模式中,进行辐射通量计算,并将计算的地面辐射通量与观测的地面辐射通量进行了对比分析。研究表明:1)利用毫米波雷达和微波辐射计数据联合反演的云参数比较可靠;2)利用SBDART模式并结合反演的云参数,可以准确实时地计算地面及其他高度层的长短波辐射通量;3)在反演的云参数中,光学厚度对地面各种辐射通量的影响是最大的,云层的光学厚度越大,到达地面的太阳短波辐射越小,地面反射短波辐射也越小。另外云底温度越高,云体向下发射的红外长波辐射越大。地面向上的长波辐射是地面温度的普朗克函数,随地面温度而变;4)云对地面的短波辐射强迫为负值,对地面有降温的作用。云对地面的长波辐射强迫是一个正值,对地面有一个增温的作用;5)云对地面的净辐射强迫随时间变化很大,它的正负与太阳高度角和云参数有关。     

基于国际大气化学-气候模式比较计划模式数据评估中国沙尘气溶胶直接辐射强迫

目前气候模式对沙尘气溶胶直接辐射强迫模拟仍有很大不确定性,多模式对比有助于定量评估不确定范围。国际大气化学—气候模式比较计划（Atmospheric Chemistry and Climate Model Intercomparison Project,ACCMIP）旨在评估当前模式对短寿命大气成分辐射强迫和气候效应的模拟能力。基于7个ACCMIP模式模拟的中国地区沙尘气溶胶浓度,我们评估了中国区域沙尘气溶胶直接辐射强迫和不确定性范围。结果显示,中国区域沙尘气溶胶年排放总量为215±163 Tg a-1,区域年均地表浓度为41±27 μg m-3,柱浓度为9±4 kg m-2,光学厚度为0.09±0.05。中国区域年均沙尘气溶胶产生的大气顶短波、长波和总辐射强迫分别为-1.3±0.8 W m-2、0.7±0.4 W m-2和-0.5±0.7 W m-2;地表短波、长波和总的辐射强迫值为-1.5±1.0 W m-2、1.8±0.9 W m-2和0.2±0.2 W m-2。沙尘气溶胶长波辐射强迫对沙尘浓度的垂直分布敏感。高层沙尘气溶胶浓度越大,其在大气顶产生更强的正值长波辐射强迫。然而,沙尘气溶胶短波辐射强迫主要受整层沙尘柱浓度控制,对沙尘浓度的垂直分布较不敏感。本文结果可为中国沙尘气溶胶的气候模拟提供参考。     

MM5 simulations of interannual change and the diurnal cycle of southern African regional climate

Summary Two cumulus convection and two planetary boundary layer schemes are used to investigate the climate of southern Africa using the MM5 regional climate model. Both a wet (1988/89) and a dry (1991/92) summer (December–February, DJF) rainfall season are simulated and the results compared with three different observational sources: Climate Research Unit seasonal data (precipitation, 2 m surface temperature, number of rain days), satellite-derived diurnal precipitation and the Surface Radiation Budget diurnal short-wave fluxes and optical depth. Using the ETA model boundary layer in MM5 simulates too much incident short-wave radiation at the surface at 12 UTC, whereas the medium range forecast model boundary layer yields a diurnal cycle of short-wave radiation closer to the observed. The Betts-Miller convection scheme in MM5 simulates peak rainfall later in the day and less rain days than observed, whereas when using the Kain-Fritsch convection scheme a peak rainfall earlier in the day and more rain days than observed are simulated. The intensity of the hydrological cycle is therefore dependent on the choice of convection scheme, which in turn is further modified by the boundary layer scheme. Precipitation during the wet 1988/89 season is reasonably captured by most simulations, though using the Betts-Miller scheme more accurately simulates rainfall during the dry 1991/92 season. Mean DJF biases in the surface temperature and diurnal temperature range are consistent with biases in the number of rain days and the diurnal cycles of surface moisture and energy.