Topographic radiation modeling and spatial scaling of clear-sky land surface longwave radiation over rugged terrain
Topographic radiation modeling and spatial scaling of clear-sky land surface longwave radiation over rugged terrain
复制标题
崎岖地形上晴空地表长波辐射的地形辐射建模和空间缩放
DOI:
10.1016/j.rse.2015.10.026
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发表时间:
2016
影响因子:
13.5
通讯作者:
Chen Ling
中科院分区:
文献类型:
--
作者:
Yan Guangjian;Wang Tianxing;Jiao Zhonghu;Mu Xihan;Zhao Jing;Chen Ling
Longwave radiation (5–100 μm) is a critical component of the Earth's radiation budget. Most of the existing satellite-based retrieval algorithms are valid only for flat surfaces without accounting for topographic effects. This causes significant errors. Meanwhile, the fixed spatial resolution of remote sensing data makes it difficult to link the satellite-derived longwave radiation to different land models running on various scales. These deficiencies result in an urgent need for topographic modeling and spatial scaling studies of longwave radiation. In this paper, a longwave topographic radiation model (LWTRM) is proposed that quantifies all possible radiation-affecting factors over rugged terrain. For driving the LWTRM, a hybrid method for simultaneously deriving multiple components of longwave radiation from MODIS data is suggested based on artificial neuron networks (ANN) and the radiative transfer simulation. Topographically corrected longwave radiation is then derived by coupling the ANN outputs and LWTRM. Based on this, a general upscaling strategy for longwave radiation is presented. The results demonstrate that: (1) both the proposed LWTRM and the upscaling strategy are rather effective and work well over rugged areas; (2) the ANN-based retrieval method can produce longwave radiation with better accuracy(RMSE < 23 W/m2, bias < 9 W/m2). More importantly, it can simultaneously derive multiple components of longwave radiation in a consistent manner; (3) over mountainous areas, the radiation cannot be accurately characterized in terms of either spatial distribution or specific values if topographic effects are neglected, for instance, the induced error can reach up to 100 W/m2for the longwave net flux; and (4) the topographic effects cannot be ignored below spatial scale of approximately 5 km in the selected study area.
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通讯作者:
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