Journal of Arid Meteorology ›› 2026, Vol. 44 ›› Issue (1): 115-125.DOI: 10.11755/j.issn.1006-7639-2026-01-0115
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DONG Qiru1,2(
), WANG Ying3, LI Yinghua1(
), YANG Xu4, LIANG Kangzhuang1
Received:2025-04-27
Revised:2025-05-28
Online:2026-02-28
Published:2026-03-25
董琪如1,2(
), 王莹3, 李英华1(
), 杨旭4, 梁康壮1
通讯作者:
李英华
作者简介:董琪如(1992—),女,高级工程师,主要从事资料同化技术及灾害性天气分析研究。E-mail: dongqiru77@163.com。
基金资助:CLC Number:
DONG Qiru, WANG Ying, LI Yinghua, YANG Xu, LIANG Kangzhuang. Causes analysis of an extreme warm-sector rainstorm in Beijing-Tianjin-Hebei region[J]. Journal of Arid Meteorology, 2026, 44(1): 115-125.
董琪如, 王莹, 李英华, 杨旭, 梁康壮. 京津冀地区一次极端暖区暴雨成因分析[J]. 干旱气象, 2026, 44(1): 115-125.
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URL: http://www.ghqx.org.cn/EN/10.11755/j.issn.1006-7639-2026-01-0115
| 物理方案 | 选项设置 |
|---|---|
| 微物理方案 | 新Tompson |
| 近地面方案 | MM5相似理论 |
| 陆面方案 | Noah |
| 行星边界层方案 | ACM2 PBL |
| 积云参数化方案 | Kain-Fritsch(d02区无) |
| 长波辐射方案 | RRTM |
| 短波辐射方案 | Dudhia |
Tab.1 Main parameterization schemes of the model
| 物理方案 | 选项设置 |
|---|---|
| 微物理方案 | 新Tompson |
| 近地面方案 | MM5相似理论 |
| 陆面方案 | Noah |
| 行星边界层方案 | ACM2 PBL |
| 积云参数化方案 | Kain-Fritsch(d02区无) |
| 长波辐射方案 | RRTM |
| 短波辐射方案 | Dudhia |
Fig.3 The 500 hPa geopotential height (contour lines,Unit: dagpm),wind field (arrow vectors,Unit: m·s-1) and 200 hPa high-level jet (the shaded,Unit: m·s-1)(a,b),and 850 hPa geopotential height (contour lines,Unit: dagpm),wind field (arrow vectors,Unit: m·s-1),and low-level jet ( the shaded,Unit: m·s-1)(c,d) at 06:00 (a,c) and 15:00 (b,d) August 12,2020
Fig.4 Distribution of observed (a,c) and simulated (b,d) accumulated precipitation at 10:00 (1 hour)(a,b) and from 09:00 to 15:00 (6 hours)(c,d) August 12,2020 (Unit: mm) (The AB line denotes the core region of the 6-hour accumulated precipitation maximum along the orientation of the rainfall belt)
Fig.5 Simulated maximum radar reflectivity (Unit: dBz) at different forecasting time from 10:00 to 15:00 on August 12,2020 (The black box represents the mesoscale convective system that influenced the rainstorm)
Fig.6 The simulated 850 hPa wind field (wind vectors,Unit: m·s-1) and divergence (the color shaded,Unit: 10-4 s-1) at 11:00 (a),13:00 (b),15:00 (c) on August 12,2020 (The black box indicates the area of strong convergence,and the ellipses represent the convergence point of the wind field)
Fig.7 The simulated vertical cross sections of wind vectors (wind vectors,Unit: m·s-1),vertical velocity (the color shaded,Unit: m·s-1) and wind velocity (isolines,Unit: m·s-1) along the AB line of the Fig.4(d) from 10:00 to 15:00 on August 12,2020 (a)10:00,(b)11:00,(c)12:00,(d)13:00,(e)14:00,(f)15:00 (The red box indicates the area where the low-level easterly wind is gradually strengthening,and the purple box indicates the intensity pulsation zone of the low-level jet)
Fig.8 The simulated vertical cross sections of potential pseudo-equivalent temperature (isolines,Unit: K) and divergence (the color shaded,Unit: 10-4s-1) along the AB line of the Fig.4(d) at 11:00 (a),13:00 (b),15:00 (c) on August 12,2020
Fig.9 The simulated water vapour fux divergence (the color shaded,Unit: 10-6 g·cm-2·hPa-1·s-1),wind field (wind vectors,Unit: m·s-1),specific humidity (green isolines,Unit: g·kg-1) and terrain height (the area filled with line segments,Unit: m) at 950 hPa at 11:00 (a),13:00 (b),15:00 (c) on August 12,2020 (The black box denotes the region of intense water vapor convergence)
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