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夏季西藏4个站点大气向下长波辐射观测分析
引用本文:刘梦琪,郑向东,赵春生. 夏季西藏4个站点大气向下长波辐射观测分析[J]. 应用气象学报, 2018, 29(5): 596-608. DOI: 10.11898/1001-7313.20180508
作者姓名:刘梦琪  郑向东  赵春生
作者单位:1.中国气象科学研究院, 北京 100081
基金项目:国家自然科学基金项目(91537213,91637107),公益性行业(气象)科研专项(GYHY201106023,GYHY201406001),中央级公益性科研院所基本科研业务费专项(2011Z003,2013Z005)
摘    要:对2011—2016年部分夏季时段分别在西藏那曲、拉萨、林芝和阿里观测的大气向下长波辐射(L)进行分析,结果显示:L具有明显的日变化,最大值出现在北京时间15:00前后,而最低值出现在凌晨至10:00,日平均值林芝最高(368 W·m-2),其次是拉萨(319 W·m-2)、阿里(305 W·m-2)和那曲(299 W·m-2)。晴天L ?ngstr?m(1915)的经验公式最适合林芝,而Konzelmann(1994)的公式则适合那曲、拉萨和阿里;随着人工观测总云量的增加,L增强趋势明显,满云(云量7~10成)情形4个站点云增强效应均从20 W·m-2上升至50 W·m-2以上,低云量对L的增强效应明显高于总云量。云份额数(CF)上升所对应天顶方向平均云底高度下降,但云增强效应上升。在晴天(CF为-5%~5%、平均云底高度大于4 km)时,云增强效应仅为5 W·m-2左右(林芝接近20 W·m-2),但当CF为90%以上(云底高度小于3.5 km)时,云增强效应则上升到60 W·m-2(林芝接近50 W·m-2)。固定云底高度,CF与L云增强效应呈显著相关(r2为0.91~0.97),远高于云底高度与L云增强效应的相关(r2为0.32~0.58)。

关 键 词:大气向下长波辐射(L)   云份额数(CF)   云增强效应
收稿时间:2018-03-01
修稿时间:2018-05-16

Observational Analysis of Summer Atmospheric Downward Longwave Radiation at 4 Sites on the Tibetan Plateau
Liu Mengqi,Zheng Xiangdong and Zhao Chunsheng. Observational Analysis of Summer Atmospheric Downward Longwave Radiation at 4 Sites on the Tibetan Plateau[J]. Journal of Applied Meteorological Science, 2018, 29(5): 596-608. DOI: 10.11898/1001-7313.20180508
Authors:Liu Mengqi  Zheng Xiangdong  Zhao Chunsheng
Affiliation:1.Chinese Academy of Meteorological Sciences, Beijing 1000812.Department of Atmospheric Science, School of Physics, Peking University, Beijing 100871
Abstract:The summer downward longwave radiation (L) observed in Naqu, Lhasa, Nyingchi and Ali is analyzed. The averaged L at 4 sites are 299, 319, 368 and 305 W·m-2, respectively. L is lower in the local morning and subsequently increases significantly in the afternoon. The mean diurnal variation at Naqu and Ali is about 30 W·m-2, while it's 9 and 19 W·m-2 in Lhasa and Nyingchi respectively. Based on solar shortwave radiation observations, a method to determine the daytime sky cloud-coverage index (cloud fraction, CF) is presented by the solar radiation comparisons between the empirically calculation for cloud-free situation and the observed. CF of -5% to 5% is assumed as daytime cloud-free situation to test the suitability of 10 empirical formula of L on the Plateau. It shows that the empirical formula of ?ngstr?m (1915) is most suitable for the Nyingchi where the vapor pressure is high, while the empirical formula of Konzelmann (1994) is most suitable for Naqu, Lhasa and Ali. Errors of the calculated daytime cloud-free L from the observed at Naqu, Lhasa, Nyingchi and Ali are 2.1%, -0.27%, -0.89% and 0.94%. The cloud-induced L enhancement effect (measured L minus the calculated cloud-free values given the surface temperature and humidity) clearly shows that the mean L enhancement effect at Naqu, Lhasa, Nyingchi and Ali are 30.8, 22.1, 38.8 and 15.6 W·m-2 with the median values of 24.4, 17.3, 42.7 and 6.8 W·m-2. With the increase of artificially visual total cloud amount, the increasing trend of L enhancement is obvious, especially when the cloud amount increase from less than 20% to 70% and above, the corresponding L enhancement effects rapidly increases from above 20 to more than 50 W·m-2 at all the 4 sites. Given the same visual cloud mount, the L enhancement effects induced by the low clouds in Lhasa and Ali are obviously higher than those induced by the total cloud. The effect from cloud coverage and height on the L enhancement is further confirmed by the aerosol lidar cloud base height at zenith direction and the CF. The decreasing cloud base height (no available cloud base height data in Lhasa) corresponding to increasing trends of CF and L enhancement is detected. The L enhancement effects are only about 5 W·m-2 with cloud-free condition, but they may rise to 60 W·m-2 when CF is above 90% (the average cloud base height is less than 3.5 km). Given the fixed cloud base height, the L enhancement obviously increases with the growth of CF. CF, significantly more than the zenith cloud base height, which affects the enhancement of L on the Tibetan Plateau.
Keywords:downward longwave radiation  cloud fraction  cloud-induced enhancement effect
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