墙面可能晴天太阳辐射小时总量的计算与分布

以卡斯特洛夫公式为理论基础,得到各朝向墙面可能晴天太阳总辐射和直接辐射小时总量的计算方案,计算了我国704个气象站各月代表日各个朝向墙面的逐时辐射值,分析其变化规律,并讨论了最大1h辐射量的全国分布。结果表明：南墙晴天最大1h辐射量随纬度升高而增大,而且在冬季其辐射量在各墙面中最大;东、西墙受纬度因素影响相对较小,在夏季其辐射量在各墙面中最大。     

我国住宅区日照标准下墙面晴天太阳辐射分析

为研究我国不同地区住宅通过垂直墙面上的窗口实际接受到的太阳辐射量空间分布特征,以卡斯特洛夫公式为基础,建立了各朝向墙面晴天太阳总辐射和直接辐射小时总量的计算方案。使用水汽压和海拔高度拟合了公式中的参数,计算了我国各地满足国家标准对住宅间距要求下的水平面和垂直墙面辐射量,并绘制了分布图。研究发现:大寒日各朝向墙面晴天最大2 h辐射量空间分布受纬度和大气透明度共同影响,青藏高原为全国高值中心,川黔地区为低值中心。在我国东部地区,与水平面辐射量随纬度增加而降低的规律相反,同样是辐射量最大的2 h日照时间,纬度越高的地区南墙面接受的太阳辐射量就越大。与南墙相比,东、西墙面接收的最大2 h辐射量明显偏小,不能发挥阳光对健康和卫生的作用。上述结果表明,从大寒日建筑底层南墙面接收的最大2 h辐射量上看,适当放宽北方地区日照间距标准具有一定可行性。     

西部山区总辐射气候学计算及分布

根据西部山区太阳总辐射的实测资料分析，指出，西部山区总辐射的气候学计算必须考虑日照，水汽分布及海拔高度的影响。为此研制了适宜于西部山区的总辐射气候学计算公式Ｑ＝Ｑ０（ａ＋ｂｓ１＋ｃｓ１＾２），进而讨论了西部山区总辐射的时，空分布。     

大气中的水汽对太阳紫外辐射消光的可能机制分析

本文给出了北京地区晴天和实际天气条件下到达地面太阳紫外总辐射的一种计算方法，分析了影响到达地面太阳紫外总辐射的各主要因子的主次贡献，重点讨论了水汽在参与大气中的光化学反应过程中，对到达地面的太阳紫外总辐射消光的可能机制。     

我国太阳总辐射气候学计算方法的再讨论

根据我国建站时间在30a以上的辐射资料以及对应的地面站日照资料，在分析太阳总辐射统计特征的基础上，讨论了总辐射气候学计算公式中a、b系数的地理分布和季节变化特征，分析了辐射气候学计算的可能误差，得到了用日照资料估算总辐射的误差范围。结果表明，太阳总辐射月总量接近正态分布特征；总辐射气候学计算公式中的a、b系数具有较明显的时空变化特征，需按不同月份确立；通过逐年观测资料计算各基本站a、b系数，再由内插求得无辐射资料测站的a、b系数，进而计算无辐射资料站的辐射总量，其误差在可接受的范围内。     

广州地区太阳分光辐射的某些变化特征

利用广州地区1985—1990年的太阳分光辐射的连续观测资料（观测角度为23°11′），研究了广州地区紫外辐射、可见光辐射（光合有效辐射）、近红外辐射的某些特征。结果指出，每年7—10月份各分光辐射及总辐射总量较大。月总辐射中可见光辐射占总辐射的百分比年平均为47.3%，相应的紫外辐射和近红外辐射分别占7.1%和45.6%。文中还分析了晴天条件下分光辐射的变化和1990年紫外辐射变化的某些特征，并分析和讨论了分光辐射与云量、日照时间等因子的相关。     

中国地区云对地气系统净辐射强迫的气候研究

本文利用地球辐射平衡试验（ERBE）和国际卫星云气候计划（ISCCP）提供的地气系统行星反射率，长波射出辐射（OLR）和云量资料，计算出中国地区年、月总云量对地气系统净辐射的强迫，分别讨论了其与总云量及地气系统晴天净辐射的关系。结果表明：地气系统净辐射云强迫与总云量有较好的抛线物关系，各月净辐射云强迫与地气系统晴天净辐射的曲线相关也很明显，如以曲线上净辐射云强迫为零时的晴天净辐射值代表各月曲线位置，则该值随天文辐射作规律性季节变化。地气系统净辐射云强迫的地理分布与总云量及地气晴天净辐射分布有关，其在各地的年变化则主要由天文因素及雨季进行退决定。     

太阳总辐射最佳倾角的时空分布

本文根据倾斜面上太阳总辐最佳倾角的角析表示式，利用平均太阳总辐射和直接辐月总量以及实际地表面反射率，计算分析了我国各月最佳倾角和最佳总辐射比的时空变化特征。同时对用天空散射辐射各同性模式计算倾斜面上总辐日总量的适用性问题亦作了简要讨论。     

丘陵山地总辐射的计算模式

本文根据对丘陵山地地形参数(平均坡向、坡度和地形遮蔽角)的数值模拟结果,应用试验观测资料,较详细地讨论了山地总辐射的理论计算模式。文中主要讨论了三个问题:山地总辐射理论模式的建立;模式参数的数值试验;模式在大别山南部局部地区的模拟结果及其分析。结果表明,山区总辐射受地形影响非常明显。本模式原则上适用于任何地区各种地形下总辐射的数值模拟。     

光合有效量子通量密度的气侯学计算

讨论了光合有效辐射（ＰＡＲ）的两种计量系统，提出了利用太阳总辐射照度估算光合有效量子通量密度的气候学公式。根据国外对昼光的观测资料，得到了ＰＡＲ能量的量子转换系数，即太阳总辐射中，ＰＡＲ每１Ｊ的能量含有４．５５μｍｏｌ的量子。在气候学计算中，可利用这个值进行ＰＡＲ的能量和量子的换算。     

盛夏副高脊线位置的变化规律及其成因分析

本文对盛夏7月份副高脊线位置的变化规律及其成因进行了分析,结果表明:副高脊线位置具有明显的低频变化,主要振荡周期为13年左右。它的变化在东亚具有明显的遥相关结构,其影响因子主要是东亚是否存在阻塞高压,黑潮区海温是否异常,菲律宾附近对流活动的强弱以及南印度副高的强弱变化。其中,东亚是否有阻塞高压存在和黑潮区海温是否异常变化,对盛夏7月份副高脊线位置的异常偏南或偏北有十分重要的影响。     

年代际气候变化研究

概括的介绍了中国科学家近几年在年代际气候变化方面的研究进展,包括中国气候的年代际变化特征,北大西洋涛动(NAO)和北太平洋涛动(NPO)与中国年代际气候变化的关系,北太平洋海面温度(SST)年代际模及其影响,大气环流系统的年代际变化以及气候突变问题.     

The Interactive Climate and Vegetation Along the Pole-Equator Belts Simulated by a Global Coupled Model

The interaction between climate and vegetation along four Pole-Equator-Pole （PEP） belts were explored using a global two-way coupled model, AVIM-GOALS, which links the ecophysiological processes at the land surface with the general circulation model （GCM）. The PEP belts are important in linking the climate change with the variation of sea and land, including terrestrial ecosystems. Previous PEP belts studies have mainly focused on the paleoclimate variation and its reconstruction. This study analyzes and discusses the interaction between modern climate and vegetation represented by leaf area index （LAI） and net primary production （NPP）. The results show that the simulated LAI variation, corresponding to the observed LAI variation, agrees with the peak-valley variation of precipitation in these belts. The annual mean NPP simulated by the coupled model is also consistent with PIK NPP data in its overall variation trend along the four belts, which is a good example to promote global ecological studies by coupling the climate and vegetation models. A large discrepancy between the simulated and estimated LAI emerges to the south of 15°N along PEP 3 and to the south of 18°S in PEP 1S, and the discrepancy for the simulated NPP and PIK data in the two regions is relatively smaller in contrast to the LAI difference. Precipitation is a key factor affecting vegetation variation, and the overall trend of LAI and NPP corresponds more obviously to precipitation variation than temperature change along most parts of these PEP belts.     

Spatial differences in seasonal variation of the upper-tropospheric jet stream in the Northern Hemisphere and its thermal dynamic mechanism

NCEP/NCAR reanalysis daily data from 1951 to 2008 are used in this study to reveal the spatial-asymmetric features in the seasonal variation of the upper-tropospheric jet stream (UTJS) and its thermal dynamic forcing mechanism. The jet occurrence percentage distribution of the UTJS demonstrates a spiral-like pattern in winter, but it is quasi-annular in summer. The jet occurrence percentage in the Eastern Hemisphere is larger than that in the Western Hemisphere, and its maximum area is located further south. The polar front jet stream (PJS) and subtropical jet stream (SJS) can be distinguished over the Northern Africa and Asian regions, whereas only one jet stream can be observed over the Western Pacific and Atlantic Ocean. Furthermore, a single peak pattern is found in the seasonal variation of the SJS occurrence frequency with the highest jet occurrence appearing in winter and the lowest in summer, while a double peak pattern is observed in the seasonal variation of the PJS occurrence, i.e., the jet occurrence reaches its peaks in autumn and spring for the PJS. Based on the thermal wind theory, air temperature gradient and atmospheric baroclinicity are calculated and compared with the jet occurrence variation to explore the thermal dynamic forcing mechanism for the UTJS variation. In addition, synoptic-scale transports of eddy heat and momentum are also calculated. The results indicate that the SJS variation is primarily determined by the air temperature gradient and atmospheric baroclinicity, while the PJS variation is under great influence of the transport of eddy heat and momentum over Northern Africa and East Asia. The UTJS variation over the area from 140E to 70W cannot be well individually explained by the air temperature gradient and atmospheric baroclinicity. Further analysis indicates that UTJS variation over this area is largely under control of combined effect of the transport of eddy heat and momentum as well as the atmospheric baroclinicity.     

Quantitative evaluation of the seasonal variations in climate model cloud regimes

An extended cloud-clustering method to assess the seasonal variation of clouds is applied to five CMIP5 models. The seasonal variation of the total cloud radiative effect (CRE) is dominated by variations in the relative frequency of occurrence of the different cloud regimes. Seasonal variations of the CRE within the individual regimes contribute much less. This is the case for both observations, models and model errors. The error in the seasonal variation of cloud regimes, and its breakdown into mean amplitude and time varying components, are quantified with a new metric. The seasonal variation of the CRE of the cloud regimes is relatively well simulated by the models in the tropics, but less well in the extra-tropics. The stratocumulus regime has the largest seasonal variation of shortwave CRE in the tropics, despite having a small magnitude in the climatological mean. Most of the models capture the temporal variation of the CRE reasonably well, with the main differences between models coming from the variation in amplitude. In the extra-tropics, most models fail to correctly represent both the amplitude and time variation of the CRE of congestus, frontal and stratocumulus regimes. The annual mean climatology of the CRE and its amplitude in the seasonal variation are both underestimated for the anvil regime in the tropics, the cirrus regime and the congestus regime in the extra-tropics. The models in this study that best capture the seasonal variation of the cloud regimes tend to have higher climate sensitivities.     

黑潮延伸体区域海表温度锋的时空变化特征分析

利用NOAA最优插值逐日海表温度资料和AVISO中心的海表高度异常资料,分析了黑潮延伸体区域的海表温度锋的时空变化特征以及导致其年代际变化可能的原因。结果表明,气候平均态的黑潮延伸体区域海表温度锋位于黑潮延伸体区域北部边缘,在143 °E和150 °E附近存在两个弯曲,SST水平梯度最大值出现在142 °E附近,强度超过4.5 ℃/(100 km),其后强度自西向东逐渐递减,在149 °E附近又出现一个较弱的大值中心,在141~153 °E范围内,海表温度锋位置的平均值为36.25 °N,强度的平均值为3.22 ℃/(100 km)。黑潮延伸体区域的海表温度锋南北位置的季节变化很弱,而其强度的季节变化非常显著。相较于较弱的季节变化,海表温度锋位置的年际和年代际的低频变化则要显著得多,其南北变化跨度超过2 °。海表温度锋强度的年际和年代际的低频变化也较强,超过4.5 ℃/(100 km)。黑潮延伸体区域的海表温度锋的变化与太平洋年代际振荡（PDO）以及北太平洋涡旋振荡（NPGO）存在显著的相关关系,NPGO和PDO在中东太平洋区域会强迫产生海表高度异常,随后向西传播,在约3年后到达黑潮延伸体区域,使该区域流场发生变化产生海洋热平流异常,最终导致海表温度锋强度发生变化。      

Seasonal variation of atmospheric 210Pb and Al in the western North Pacific region

The atmospheric concentration of ²¹⁰Pb was determined for two years at six stations in the western North Pacific region. The following results were obtained and discussed by comparing them with those of Al. The atmospheric concentration of ²¹⁰Pb varied widely from week to week, but the degree of variation was about a half that of Al. Contrary to Al, the year-to-year variation of ²¹⁰Pb was not pronounced and its seasonal variation was well expressed by a sine curve. The ²¹⁰Pb concentration did not show a marked latitudinal variation and its base-line concentration was high in the surface air over the North Pacific. These suggest that atmospheric ²¹⁰Pb has a longer residence time, due to its transportation through higher altitudes and deposits much more evenly onto the Earth's surface and the ocean, as compared with Al in mineral dust which is larger in size in the source region.     

中国降水异常的特征分析

异常降水直接影响着农业和其他生产活动。文中计算分析了中国160个测站的一些反映降水变化的常规统计量,认为这些统计量难以反映出降水异常的变化特征。文中从非线性动力学和统计学相结合的角度出发,分析了相隔1～20 a间不同时间尺度的降水变率之间的关系,找到可以区分任意地区降水异常特点的特征参数,由此可进一步判断某个地区旱涝灾害发生的可能性以及强度的大小,为气候研究工作提供必要的依据。     

青藏高原及周边地区近地层小气候特征分析

利用中国气象局成都高原气象研究所建立的5个边界层站（湄潭、巴中、什邡、曲麻莱、狮泉河）2019年的观测资料，对比分析青藏高原及周边地区近地层大气要素变化和陆—气能量交换特征及异同点，探讨其原因。结果表明：（1）青藏高原及周边地区近地层大气温度、相对湿度、风速、感热通量、潜热通量、动量通量均符合一峰一谷的常规日变化特征，气压具有双峰双谷的日变化特征。（2）高海拔台站近地层温度日变幅（12℃）高于周边低海拔地区（4～6℃），季变幅与海拔高度的关系不显著。（3）相对湿度与温度关系密切，相对湿度的垂直结构和日变化都具有明显的区域差异，其垂直梯度夜间显著高于白天，峰值出现时间随夏、秋、春、冬季呈现季节性滞后，而谷值超前。（4）风速春季较大，夏、秋季次之，冬季小，季变幅略小于日变幅；低海拔区域的风速及其日变幅均显著低于高海拔区域。（5）低海拔区域气压季变幅（>13 hPa）远高于日变幅（2.5 hPa左右），而高海拔区域气压季变幅（>3 hPa）略低于日变幅（2 hPa左右）。（6）感热通量春季大、冬季小；感热通量和动量通量在高海拔区域均较高，二者具有较一致的日、季变化特征，表明大气动...     

东亚高空急流协同变化研究新进展

东亚高空急流是东亚大气环流系统的重要组成部分,对东亚地区的天气和气候具有重要影响。以往对东亚高空急流的研究多关注副热带急流及其对天气气候的影响,近年来,学者们在明确区分东亚副热带急流和极锋急流的基础上,从东亚副热带急流和极锋急流协同变化的视角,对东亚高空急流的变化规律和机理及其对我国气候异常的影响,开展了一系列研究,揭示出副热带急流和极锋急流强度的反位相协同变化是以副热带急流强（弱）伴随着极锋急流弱（强）为其主要配置形式和模态,并对应着特定的大气环流形势以及相应的气温和降水异常分布,与冬季冷空气活动、梅雨期降水、极端事件、冬季风等具有密切关系。本文聚焦东亚高空急流协同变化方面的最新研究成果,从东亚高空急流协同变化规律、高空急流协同变化的热力和动力学影响机理、高空急流协同变化气候效应、高空急流与中高纬低频遥相关型的联系等方面进行较为全面的总结,以加深东亚高空急流活动基本特征和变化规律的认识。