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2021年保定清苑EF2级龙卷S和X波段雷达特征

陈雪娇 花家嘉 裴宇杰 王振超 刘姝 刘姝君 王福侠

陈雪娇, 花家嘉, 裴宇杰, 等. 2021年保定清苑EF2级龙卷S和X波段雷达特征. 应用气象学报, 2024, 35(5): 564-576. DOI:  10.11898/1001-7313.20240505..
引用本文: 陈雪娇, 花家嘉, 裴宇杰, 等. 2021年保定清苑EF2级龙卷S和X波段雷达特征. 应用气象学报, 2024, 35(5): 564-576. DOI:  10.11898/1001-7313.20240505.
Chen Xuejiao, Hua Jiajia, Pei Yujie, et al. S-band and X-band radar observation characteristics of EF2 tornado at Qingyuan of Baoding in 2021. J Appl Meteor Sci, 2024, 35(5): 564-576. DOI:   10.11898/1001-7313.20240505.
Citation: Chen Xuejiao, Hua Jiajia, Pei Yujie, et al. S-band and X-band radar observation characteristics of EF2 tornado at Qingyuan of Baoding in 2021. J Appl Meteor Sci, 2024, 35(5): 564-576. DOI:   10.11898/1001-7313.20240505.

2021年保定清苑EF2级龙卷S和X波段雷达特征

DOI: 10.11898/1001-7313.20240505
资助项目: 

中国气象科学研究院灾害天气国家重点实验室开放课题 2023LASW-B07

南京气象科技创新研究院北极阁开放研究基金项目 BJG202409

中国气象局创新发展专项 CXFZ2023J012

河北省科技厅重点研发计划社会公共事业创新专项 23375401D

河北省气象局青年基金项目 22ky27

详细信息
    通信作者:

    裴宇杰, 邮箱: 81048870@qq.com

S-band and X-band Radar Observation Characteristics of EF2 Tornado at Qingyuan of Baoding in 2021

  • 摘要: 利用石家庄S波段天气雷达(SPOL)、雄安X波段相控阵雷达(XPAR)、地面自动气象站等多源观测资料, 分析2021年7月21日河北省保定市清苑区东吕村EF2级龙卷雷达特征。清苑区龙卷发生于低涡降水云系中, 风暴后向传播造成的多单体合并形成超级单体, 钩状回波顶部分裂的强反射率因子核心自东南向西北移动, 并与龙卷位置对应关系较好。SPOL和XPAR平均径向速度图上均连续多个时次识别出中气旋, 中气旋尺度为1.4~4.2 km, 旋转速度为10~20 m·s-1, 为弱中气旋, 属于微型超级单体龙卷, 持续时间较短(30~35 min)。在龙卷发展演变过程中, 低仰角探测到紧邻的旋转速度对时, 中气旋向下延伸1.2~1.4 km, 直径迅速收缩0.8~1 km, 预示龙卷的发生。龙卷风暴在低层旋转速度和涡度最大, 有利于龙卷发展增强。SPOL和XPAR在龙卷位置、径向速度及风暴直径的探测结果较为一致, XPAR回波顶比SPOL高约6 km, 且XPAR回波顶的峰值时段与风暴出现冲云顶特征的时段一致。15:36—15:42(北京时)龙卷涡旋特征(TVS)最为强盛, 垂直伸展厚度达2~4 km。
  • 图  1  年7月21日河北省保定市清苑区东吕村龙卷照片

    Fig. 1  Photo of tornado at Donglü Village, Qingyuan District, Baoding City, Hebei Province on 21 Jul 2021

    图  1  年7月21日河北省保定市清苑区东吕村龙卷照片

    Fig. 1  Photo of tornado at Donglü Village, Qingyuan District, Baoding City, Hebei Province on 21 Jul 2021

    图  2  年7月21日08:00 500 hPa高度(蓝线,单位:hPa)、500 hPa温度(红虚线,单位:℃)和850 hPa风场(风羽) (a)及地面气压场(蓝线,单位:hPa) 和风场(风羽) (b)

    Fig. 2  hPa geopotential height (the blue contour, unit: hPa), 500 hPa temperature (the red dashed line, unit: ℃) with 850 hPa wind (the barb) (a) and pressure (the blue contour, unit: hPa) with wind (the barb) at the surface(b) at 0800 BT 21 Jul 2021

    图  2  年7月21日08:00 500 hPa高度(蓝线,单位:hPa)、500 hPa温度(红虚线,单位:℃)和850 hPa风场(风羽) (a)及地面气压场(蓝线,单位:hPa) 和风场(风羽) (b)

    Fig. 2  hPa geopotential height (the blue contour, unit: hPa), 500 hPa temperature (the red dashed line, unit: ℃) with 850 hPa wind (the barb) (a) and pressure (the blue contour, unit: hPa) with wind (the barb) at the surface(b) at 0800 BT 21 Jul 2021

    图  3  年7月21日08:00—22日08:00清苑站物理要素时间-高度分布(填色为比湿,折线为垂直速度(单位:Pa·s-1),风羽为风场)

    Fig. 3  Time-height section of physical elements at Qingyuan Station from 0800 BT 21 Jul to 0800 BT 22 Jul in 2021 (the shaded denotes specific humidity, the curve denotes vertical velocity(unit: Pa·s-1) and the barb denotes wind)

    图  3  年7月21日08:00—22日08:00清苑站物理要素时间-高度分布(填色为比湿,折线为垂直速度(单位:Pa·s-1),风羽为风场)

    Fig. 3  Time-height section of physical elements at Qingyuan Station from 0800 BT 21 Jul to 0800 BT 22 Jul in 2021 (the shaded denotes specific humidity, the curve denotes vertical velocity(unit: Pa·s-1) and the barb denotes wind)

    图  4  年7月21日清苑区东吕村上空石家庄SPOL 0.5°仰角钩状回波特征

    Fig. 4  Hook shaped echoes over Donglü Village, Qingyuan at 0.5° elevtion of Shijiazhuang SPOL on 21 Jul 2021

    图  4  年7月21日清苑区东吕村上空石家庄SPOL 0.5°仰角钩状回波特征

    Fig. 4  Hook shaped echoes over Donglü Village, Qingyuan at 0.5° elevtion of Shijiazhuang SPOL on 21 Jul 2021

    图  5  年7月21日15:48 SPOL反射率因子及径向速度

    Fig. 5  Reflectivity factor and radial velocity of SPOL at 1548 BT 21 Jul 2021

    图  5  年7月21日15:48 SPOL反射率因子及径向速度

    Fig. 5  Reflectivity factor and radial velocity of SPOL at 1548 BT 21 Jul 2021

    图  6  年7月21日15:48 SPOL和15:44 XPAR组合反射率因子及径向速度对比(a)SPOL组合反射率因子,(b)XPAR组合反射率因子,(c)SPOL 0.5°仰角径向速度,(d)XPAR 3.0°仰角径向速度

    Fig. 6  Comparison of combined reflectivity factor and radial velocity of SPOL at 1548 BT and XPAR at 1544 BT on 21 Jul 2021(a)combined reflectivity factor of SPOL, (b)combined reflectivity factor of XPAR, (c)radial velocity at 0.5° elevation of SPOL, (d)radial velocity at 3.0° elevation of XPAR

    图  6  年7月21日15:48 SPOL和15:44 XPAR组合反射率因子及径向速度对比(a)SPOL组合反射率因子,(b)XPAR组合反射率因子,(c)SPOL 0.5°仰角径向速度,(d)XPAR 3.0°仰角径向速度

    Fig. 6  Comparison of combined reflectivity factor and radial velocity of SPOL at 1548 BT and XPAR at 1544 BT on 21 Jul 2021(a)combined reflectivity factor of SPOL, (b)combined reflectivity factor of XPAR, (c)radial velocity at 0.5° elevation of SPOL, (d)radial velocity at 3.0° elevation of XPAR

    图  7  年7月21日15:51:30 XPAR径向速度

    Fig. 7  Radial velocity of XPAR at 155130 BT 21 Jul 2021

    图  7  年7月21日15:51:30 XPAR径向速度

    Fig. 7  Radial velocity of XPAR at 155130 BT 21 Jul 2021

    图  8  年7月21日15:30—16:00 SPOL和XPAR探测龙卷风暴单体参数(a)最大反射率因子,(b)最大反射率因子所在高度,(c)垂直积分液态水含量,(d)回波顶高

    Fig. 8  Tornado storm parameters of SPOL and XPAR from 1530 BT to 1600 BT on 21 Jul 2021(a)maximum reflectivity factor, (b)height of maximum reflectivity factor, (c)vertical integrated liquid water content, (d)echo top height

    图  8  年7月21日15:30—16:00 SPOL和XPAR探测龙卷风暴单体参数(a)最大反射率因子,(b)最大反射率因子所在高度,(c)垂直积分液态水含量,(d)回波顶高

    Fig. 8  Tornado storm parameters of SPOL and XPAR from 1530 BT to 1600 BT on 21 Jul 2021(a)maximum reflectivity factor, (b)height of maximum reflectivity factor, (c)vertical integrated liquid water content, (d)echo top height

    图  9  年7月21日15:30—16:00不同仰角SPOL和XPAR中气旋最大正负速度

    Fig. 9  Maximum positive and negative velocities of mesocyclone with different elevation angles of SPOL and XPAR from 1530 BT to 1600 BT on 21 Jul 2021

    图  9  年7月21日15:30—16:00不同仰角SPOL和XPAR中气旋最大正负速度

    Fig. 9  Maximum positive and negative velocities of mesocyclone with different elevation angles of SPOL and XPAR from 1530 BT to 1600 BT on 21 Jul 2021

    图  10  年7月21日SPOL和XPAR探测龙卷中气旋低仰角旋转速度及最大涡度

    Fig. 10  Low elevation rotation velocity and the maximum vorticity of mesocyclone from SPOL and XPAR on 21 Jul 2021

    图  10  年7月21日SPOL和XPAR探测龙卷中气旋低仰角旋转速度及最大涡度

    Fig. 10  Low elevation rotation velocity and the maximum vorticity of mesocyclone from SPOL and XPAR on 21 Jul 2021

    图  11  年7月21日XPAR探测龙卷中气旋(a)及TVS参数(b)

    Fig. 11  Mesocyclone(a) and TVS parameters(b) of XPAR on 21 Jul 2021

    图  11  年7月21日XPAR探测龙卷中气旋(a)及TVS参数(b)

    Fig. 11  Mesocyclone(a) and TVS parameters(b) of XPAR on 21 Jul 2021

    表  1  中气旋特征参数统计表

    Table  1  Statistical table of characteristic parameters of mesocyclone

    仰角/(°) 旋转速度/(m·s-1) 涡度/s-1 直径/km
    XPAR SPOL XPAR SPOL XPAR SPOL XPAR SPOL
    0.0 0.5 12.8 11.0 12.4 10.4 4.8 4.7
    1.5 1.5 13.2 11.1 13.0 9.1 4.9 5.1
    3.0 2.4 13.8 8.8 12.0 8.0 5.3 4.6
    4.5 3.4 13.6 7.1 12.2 9.3 5.3 3.8
    6.0 4.3 13.6 8.3 10.5 8.5 6.1 3.6
    7.5 6.0 12.5 5.8 11.6 3.8 5.2 5.8
    下载: 导出CSV

    表  1  中气旋特征参数统计表

    Table  1  Statistical table of characteristic parameters of mesocyclone

    仰角/(°) 旋转速度/(m·s-1) 涡度/s-1 直径/km
    XPAR SPOL XPAR SPOL XPAR SPOL XPAR SPOL
    0.0 0.5 12.8 11.0 12.4 10.4 4.8 4.7
    1.5 1.5 13.2 11.1 13.0 9.1 4.9 5.1
    3.0 2.4 13.8 8.8 12.0 8.0 5.3 4.6
    4.5 3.4 13.6 7.1 12.2 9.3 5.3 3.8
    6.0 4.3 13.6 8.3 10.5 8.5 6.1 3.6
    7.5 6.0 12.5 5.8 11.6 3.8 5.2 5.8
    下载: 导出CSV
  • [1] 俞小鼎. 多普勒天气雷达原理与业务应用. 北京: 气象出版社, 2006.

    Yu X D. Principle and Operational Application of Doppler Weather Radar. Beijing: China Meteorological Press, 2006.
    [2] 冯佳玮, 闵锦忠, 庄潇然. 中国龙卷时空分布及其环境物理量特征. 热带气象学报, 2017, 33(4): 530-539.

    Feng J W, Min J Z, Zhuang X R. The spatial and temporal distribution of Chinese tornados and their characteristics analysis of environmental physical variations. J Trop Meteor, 2017, 33(4): 530-539.
    [3] 白华, 袁潮, 潘晓, 等. 辽宁省温带气旋龙卷的环境参数特征. 应用气象学报, 2023, 34(1): 104-116. doi:  10.11898/1001-7313.20230109

    Bai H, Yuan C, Pan X, et al. Environmental characteristics of extratropical cyclone tornadoes in Liaoning. J Appl Meteor Sci, 2023, 34(1): 104-116. doi:  10.11898/1001-7313.20230109
    [4] 王一童, 王秀明, 俞小鼎. 产生致灾大风的超级单体回波特征. 应用气象学报, 2022, 33(2): 180-191. doi:  10.11898/1001-7313.20220205

    Wang Y T, Wang X M, Yu X D. Radar characteristics of straight-line damaging wind producing supercell storms. J Appl Meteor Sci, 2022, 33(2): 180-191. doi:  10.11898/1001-7313.20220205
    [5] 俞小鼎. 雷暴与强对流临近预报. 北京: 气象出版社, 2020.

    Yu X D. Thunderstorm and Strong Convection Prediction. Beijing: China Meteorological Press, 2020.
    [6] Johns R H, Doswell C A Ⅲ. Severe local storms forecasting. Wea Forecasting, 1992, 7(4): 588-612. doi:  10.1175/1520-0434(1992)007<0588:SLSF>2.0.CO;2
    [7] Davies-Jones R, Trapp R J, Bluestein H B. Tornadoes and tornadic storms. Meteor Monogr, 2001, 28: 167-221.
    [8] Moller A R. Severe Local Storms Forecasting//Severe Convective Storms. Boston, MA: American Meteorological Society, 2001: 433-480.
    [9] Goodnight J S, Chehak D A, Trapp R J. Quantification of QLCS tornado genesis associated characteristics, and environments across a large sample. Wea Forecasting, 2022, 37 (11): 2087-2105. doi:  10.1175/WAF-D-22-0016.1
    [10] Wilson J W, Reum D. The flare echo: Reflectivity and velocity signature. J Atmos Oceanic Technol, 1988, 5(2): 197-205. doi:  10.1175/1520-0426(1988)005<0197:TFERAV>2.0.CO;2
    [11] Wilson J W, Roberts R D. Summary of convective storm initiation and evolution during IHOP: Observational and modeling perspective. Mon Wea Rev, 2006, 134(1): 23-47. doi:  10.1175/MWR3069.1
    [12] Davies-Jones R. A review of supercell and tornado dynamics. Atmos Res, 2015, 158: 274-291.
    [13] Fischer J, Dahl J M L, Coffer B E, et al. Supercell tornadogenesis: Recent progress in our state of understanding. Bull Amer Meteor Soc, 2024, 105(7): E1084-E1097. doi:  10.1175/BAMS-D-23-0031.1
    [14] Coffer B E, Parker M, Peters J, et al. Supercell low-level mesocyclones: Origins of inflow and vorticity. Mon Wea Rev, 2023, 151(9): 2205-2232. doi:  10.1175/MWR-D-22-0269.1
    [15] 郑媛媛, 朱红芳, 方翔, 等. 强龙卷超级单体风暴特征分析与预警研究. 高原气象, 2009, 28(3): 617-625.

    Zheng Y Y, Zhu H F, Fang X, et al. Characteristic analysis and early-warning of tornado supercell storm. Plateau Meteor, 2009, 28(3): 617-625.
    [16] 黄先香, 俞小鼎, 炎利军, 等. 广东两次台风龙卷的环境背景和雷达回波对比. 应用气象学报, 2018, 29(1): 70-83. doi:  10.11898/1001-7313.20180107

    Huang X X, Yu X D, Yan L J, et al. Contrastive analysis of two intense typhoon-tornado cases with synoptic and Doppler weather radar data in Guangdong. J Appl Meteor Sci, 2018, 29(1): 70-83. doi:  10.11898/1001-7313.20180107
    [17] 王宁, 王婷婷, 张硕, 等. 东北冷涡背景下一次龙卷过程的观测分析. 应用气象学报, 2014, 25(4): 463-469. doi:  10.3969/j.issn.1001-7313.2014.04.009

    Wang N, Wang T T, Zhang S, et al. Observation of a tornado in the birculation background of Northeast bold vortex. J Appl Meteor Sci, 2014, 25(4): 463-469. doi:  10.3969/j.issn.1001-7313.2014.04.009
    [18] 杨伟, 方阳, 蒋帅, 等. 2017年8月13日东洞庭湖水龙卷特征. 应用气象学报, 2020, 31(3): 328-338. doi:  10.11898/1001-7313.20200307

    Yang W, Fang Y, Jiang S, et al. Characteristics of the waterspout in East Dongting Lake on 13 August 2017. J Appl Meteor Sci, 2020, 31(3): 328-338. doi:  10.11898/1001-7313.20200307
    [19] Parker M D. Composite VORTEX2 supercell environments from near-storm soundings. Mon Wea Rev, 2014, 142(2): 508-529. doi:  10.1175/MWR-D-13-00167.1
    [20] Coffer B E, Parker M D, Thompson R L, et al. Using near-ground storm relative helicity in supercell tornado forecasting. Wea Forecasting, 2019, 34(5): 1417-1435. doi:  10.1175/WAF-D-19-0115.1
    [21] Coffer B E, Taszarek M, Parker M D. Near-ground wind profiles of tornadic and nontornadic environments in the United States and Europe from ERA5 reanalyses. Wea Forecasting, 2020, 35(6): 2621-2638. doi:  10.1175/WAF-D-20-0153.1
    [22] Nixon C J, Allen J T. Distinguishing between hodographs of severe hail and tornadoes. Wea Forecasting, 2022, 37(10): 1761-1782. doi:  10.1175/WAF-D-21-0136.1
    [23] 傅佩玲, 胡东明, 黄浩, 等. 台风山竹(1822)龙卷的双极化相控阵雷达特征. 应用气象学报, 2020, 31(6): 706-718. doi:  10.11898/1001-7313.20200606

    Fu P L, Hu D M, Huang H, et al. Observation of a tornado event in outside-region of Typhoon Mangkhut by X-band polarimetric phased array radar in 2018. J Appl Meteor Sci, 2020, 31(6): 706-718. doi:  10.11898/1001-7313.20200606
    [24] 徐玥, 邵美荣, 唐凯, 等. 2021年黑龙江两次超级单体龙卷过程多尺度特征. 应用气象学报, 2022, 33(3): 305-318.

    Xu Y, Shao M R, Tang K, et al. Multiscale characteristics of two supercell tornados of Heilongjiang in 2021. J Appl Meteor Sci, 2022, 33(3): 305-318.
    [25] 何彩芬, 姚秀萍, 胡春蕾, 等. 一次台风前部龙卷的多普勒天气雷达分析. 应用气象学报, 2006, 17(3): 370-375. doi:  10.3969/j.issn.1001-7313.2006.03.015

    He C F, Yao X P, Hu C L, et al. Analyses on a tornado event in front of a typhoon. J Appl Meteor Sci, 2006, 17(3): 370-375. doi:  10.3969/j.issn.1001-7313.2006.03.015
    [26] 郭飞燕, 刁秀广, 褚颖佳, 等. 弱垂直风切变环境下强下击暴流双偏振雷达特征. 应用气象学报, 2023, 34(6): 681-693. doi:  10.11898/1001-7313.20230604

    Guo F Y, Diao X G, Chu Y J, et al. Dual polarization radar characteristics of severe downburst occurred in weak vertical wind shear. J Appl Meteor Sci, 2023, 34(6): 681-693. doi:  10.11898/1001-7313.20230604
    [27] Browning K A. Cellular structures of convective storms. Metero Mag, 1962, 91: 341-350.
    [28] Browning K A. The growth of large hail within a steady updraught. Q J R Meteor Soc, 1963, 89(382): 490-506. doi:  10.1002/qj.49708938206
    [29] Browning K A. Airflow and precipitation trajectories within severe local storms which travel to the right of the winds. J Atmos Sci, 1964, 21(6): 634-639. doi:  10.1175/1520-0469(1964)021<0634:AAPTWS>2.0.CO;2
    [30] 吴翀, 刘黎平, 汪旭东, 等. 相控阵雷达扫描方式对回波强度测量的影响. 应用气象学报, 2014, 25(4): 406-414. doi:  10.3969/j.issn.1001-7313.2014.04.003

    Wu C, Liu L P, Wang X D, et al. The measurement influence of reflectivity factor caused by scanning mode from phased array radar. J Appl Meteor Sci, 2014, 25(4): 406-414. doi:  10.3969/j.issn.1001-7313.2014.04.003
    [31] 王超, 吴翀, 刘黎平. X波段双线偏振雷达数据质量分析及控制方法. 高原气象, 2019, 38(3): 636-649.

    Wang C, Wu C, Liu L P. Data quality analysis and control method of X-band dual polarization radar. Plateau Meteor, 2019, 38(3): 636-649.
    [32] 陈强, 柯杭, 赖绍钧, 等. 福州地区X波段相控阵雷达与S波段机械雷达回波数据对比分析. 海峡科学, 2022(12): 7-12. doi:  10.3969/j.issn.1673-8683.2022.12.003

    Chen Q, Ke H, Lai S J, et al. Comparative analysis of echo data between X-band phased array radar and S-band mechanical radar in Fuzhou Area. Straits Sci, 2022(12): 7-12. doi:  10.3969/j.issn.1673-8683.2022.12.003
    [33] 张曦, 黄兴友, 刘新安, 等. 北京大兴国际机场相控阵雷达强对流天气监测. 应用气象学报, 2022, 33(2): 192-204. doi:  10.11898/1001-7313.20220206

    Zhang X, Huang X Y, Liu X A, et al. The hazardous convective storm monitoring of phased-array antenna radar at Daxing International Airport of Beijing. J Appl Meteor Sci, 2022, 33(2): 192-204. doi:  10.11898/1001-7313.20220206
    [34] 张妤晴, 张伟, 郑辉, 等. S波段-X波段雷达联合观测在厦门局地短时强降水过程中的应用分析. 气象与环境科学, 2023, 46(4): 85-94.

    Zhang Y Q, Zhang W, Zheng H, et al. Application analysis of S-POL-XPAR joint observation in local short-time heavy precipitation processes in Xiamen. Meteor Environ Sci, 2023, 46(4): 85-94.
    [35] 苏永彦, 刘黎平. S波段双偏振雷达和X波段相控阵天气雷达中气旋识别结果对比. 气象, 2022, 48(2): 229-244.

    Su Y Y, Liu L P. Comparison of mesocyclone identification results between S-band dual polarization radar and X-band phased array weather radar. Meteor Mon, 2022, 48(2): 229-244.
    [36] 郑永光, 朱文剑, 姚聃, 等. 风速等级标准与2016年6月23日阜宁龙卷强度估计. 气象, 2016, 42(11): 1289-1303. doi:  10.7519/j.issn.1000-0526.2016.11.001

    Zheng Y G, Zhu W J, Yao D, et al. Wind speed scales and rating of the intensity of the 23 June 2016 tornado in Funing County, Jiangsu Province. Meteor Mon, 2016, 42(11): 1289-1303. doi:  10.7519/j.issn.1000-0526.2016.11.001
    [37] 章国材. 强对流天气分析与预报. 北京: 气象出版社, 2011.

    Zhang G C. Analysis and Forecast of Severe Convective Weather. Beijing: China Meteorological Press, 2011.
    [38] Lee R R, White A. Improvement of the WSR-88D mesocyclone algorithm. Wea Forecasting, 1998, 13(2): 341-351. doi:  10.1175/1520-0434(1998)013<0341:IOTWMA>2.0.CO;2
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  • 收稿日期:  2024-05-25
  • 修回日期:  2024-08-14
  • 刊出日期:  2024-09-30

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