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Sensitivity of convective precipitation to model grid spacing and land-surface resolution in ICON
Quarterly Journal of the Royal Meteorological Society ( IF 3.0 ) Pub Date : 2021-05-02 , DOI: 10.1002/qj.4046
Shweta Singh 1 , Norbert Kalthoff 1 , Leonhard Gantner 1
Affiliation  

The impact of model grid spacing and land-surface resolution (LSR) on convective precipitation are investigated for areas with different orographic complexities. ICOsahedral Nonhydrostatic (ICON) model simulations were performed for six days having weak large-scale forcing using six model grid spacings (in metres): Numerical Weather Prediction (NWP) ( Δ 5000 , Δ 2500 ) and Large-Eddy Simulation (LES) physics simulations ( Δ 1250 , Δ 625 , Δ 312 , and Δ 156 ) in a nested set-up. Concerning LSR, we focused on simulations with LSRs of 1,250 and 5,000 m, keeping the model grid spacing at 156 m. The onset of precipitation in Δ 1250 is earlier by 0.5–2 hr, while LSR modifications show a similar onset compared with Δ 156 . The relative percentage difference (RPD) of areal mean daily precipitation across LES physics simulations decreases consistently with model grid spacing for most of the cases. The RPD of precipitation in Δ 1250 is considerably higher (75th percentile: ≈155%) than that of the LSR runs at resolutions of both 1,250 and 5,000 m, with 75th percentiles of ≈7% and ≈22%, respectively. To investigate the processes causing the differences in precipitation characteristics, like onset time and amount, the heat and moisture budgets of Δ 1250 and Δ 156 were compared. The results show that, at the initial stage of cloud formation, a higher number of smaller clouds are formed in Δ 156 compared with Δ 1250 . The small clouds in Δ 156 are subject to considerable evaporative cooling at their edges and shell regions, due to entrainment processes. As a result, these clouds often dissolve before they can grow deep. Later on, cloud aggregation in Δ 156 also enables precipitation. The delayed onset of precipitation and reduced areas of aggregated clouds having low precipitation rates are the main reasons for less precipitation in Δ 156 than in Δ 1250 .

中文翻译:

对流降水对 ICON 模型网格间距和地表分辨率的敏感性

针对具有不同地形复杂性的地区,研究了模型网格间距和地表分辨率 (LSR) 对对流降水的影响。ICOsahedral Nonhydrostatic (ICON) 模型模拟使用六个模型网格间距(以米为单位)进行了六天的弱大规模强迫:数值天气预报 (NWP) ( Δ 5000 , Δ 2500 ) 和大涡模拟 (LES) 物理模拟 ( Δ 1250 , Δ 625 , Δ 312 , 和 Δ 156 ) 在嵌套设置中。关于 LSR,我们专注于使用 1,250 和 5,000 m 的 LSR 进行模拟,将模型网格间距保持在 156 m。降水的开始 Δ 1250 提前 0.5-2 小时,而 LSR 修改显示与 Δ 156 . 在大多数情况下,LES 物理模拟中区域平均日降水量的相对百分比差异 (RPD) 与模型网格间距一致减小。降水的 RPD Δ 1250 比 LSR 在 1,250 和 5,000 m 的分辨率下运行的要高得多(第 75 个百分位数:≈155%),第 75 个百分位数分别为 ≈7% 和 ≈22%。调查导致降水特征差异的过程,如开始时间和数量,热量和水分收支 Δ 1250 Δ 156 进行了比较。结果表明,在云形成的初始阶段,更多较小的云形成于 Δ 156 和....相比 Δ 1250 . 里面的小云 Δ 156 由于夹带过程,它们的边缘和壳区域受到相当大的蒸发冷却。结果,这些云通常在它们变得更深之前就溶解了。后来,云聚合在 Δ 156 还可以进行降水。降水的延迟和低降水率的云团面积减少是造成我国降水偏少的主要原因。 Δ 156 比在 Δ 1250 .
更新日期:2021-05-02
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