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不同类型九龙涡的水汽输送与热力结构特征的对比分析

屈顶 李跃清 李娟 范旭燕

屈顶, 李跃清, 李娟, 等. 2023. 不同类型九龙涡的水汽输送与热力结构特征的对比分析[J]. 大气科学, 47(5): 1481−1494 doi: 10.3878/j.issn.1006-9895.2208.21202
引用本文: 屈顶, 李跃清, 李娟, 等. 2023. 不同类型九龙涡的水汽输送与热力结构特征的对比分析[J]. 大气科学, 47(5): 1481−1494 doi: 10.3878/j.issn.1006-9895.2208.21202
QU Ding, LI Yueqing, LI Juan, et al. 2023. Comparative Analysis of Water Vapor Transport and Thermodynamic Characteristics of Different Types of Jiulong Vortices Found in Southwest China [J]. Chinese Journal of Atmospheric Sciences (in Chinese), 47(5): 1481−1494 doi: 10.3878/j.issn.1006-9895.2208.21202
Citation: QU Ding, LI Yueqing, LI Juan, et al. 2023. Comparative Analysis of Water Vapor Transport and Thermodynamic Characteristics of Different Types of Jiulong Vortices Found in Southwest China [J]. Chinese Journal of Atmospheric Sciences (in Chinese), 47(5): 1481−1494 doi: 10.3878/j.issn.1006-9895.2208.21202

不同类型九龙涡的水汽输送与热力结构特征的对比分析

doi: 10.3878/j.issn.1006-9895.2208.21202
基金项目: 国家自然科学基金重大研究计划集成项目91937301,国家自然科学基金重点项目42030611,重庆市气象局青年基金项目QNJJ-202211
详细信息
    作者简介:

    屈顶,女,1995年出生,硕士研究生,主要从事高原天气研究。E-mail: 18280083400@163.com

    通讯作者:

    李跃清,E-mail: yueqingli@163.com

  • 中图分类号: P443

Comparative Analysis of Water Vapor Transport and Thermodynamic Characteristics of Different Types of Jiulong Vortices Found in Southwest China

Funds: National Natural Science Foundation of China’s Major Research Project Integration Project (Grant 91937301), National Natural Science Foundation of China Key Project (Grant 42030611), Youth Fund Project of Chongqing Meteorological Bureau (Grant QNJJ-202211)
  • 摘要: 应用1989~2018年6~8月ERA-interim再分析资料,在西南涡之九龙涡新定义的基础上,通过观测、诊断、合成分析,深入研究了川西高原涡源子区域1和子区域2源地型、偏东型、东北型、偏南型九龙涡的水汽输送、热力特征及其变化。结果表明:(1)夏季九龙涡水汽主要来源于印度洋,受多尺度系统协同作用影响,源地型、偏东型、东北型生成区主要为西南水汽输送,偏南型则为西北水汽输送。伴随九龙涡生成,生成区水汽辐合逐渐加强,结束时次,移动型九龙涡在对应的移动方向下游具有异常的水汽通量辐合。(2)九龙涡涡区主要为热量消耗,其中源地型九龙涡热量消耗较大且无充足补给成为其消亡的原因之一,初生时次低层(高层)水汽消耗(增加),但发展后均为消耗;子区域1(子区域2)下垫面、环流影响复杂(简单),视热源、视水汽汇项垂直分布多样(单一),具有多个(一个)极值中心;辐射冷却和小尺度涡旋垂直输送可使视热源项中心高于视水汽汇项中心。(3)九龙涡的视热源、视水汽汇的大值区主要位于低涡东北部,且视水汽汇强于视热源,分别对应低涡强对流区和强夜发性;移动型的视热源和视水汽汇分布及变化一般都强于源地型,其中,子区域1的东北型、偏南型始终保持较强分布,子区域2的移动型和源地型初生时次差异不大,结束时次东北型显著增强。(4)源地型低涡的消亡最先表现为视水汽汇在低涡外围的减弱,而偏东型、东北型则在移动方向扩展、增强,形成视热源、水汽汇大值区,分别预示着九龙涡的减弱消亡和发展移动;偏南型西南侧有一热源大值系统,可能成为其偏南移出的外强迫因素。综上,区域和环境水汽、大气热力条件等异常变化与九龙涡演变密切相关,两者可能是九龙涡生成、消亡、发展、移动的重要原因。
  • 图  1  1989~2018年6~8月不同类型九龙涡的空间分布情况(黑色实心圆:源地型,红色实心圆:偏东型,蓝色实心圆:东北型,绿色实心圆:偏南型,不同大小实心圆表示不同频次)

    Figure  1.  Spatial distributions of different JLVs (Jiulong vortexs) during June–August from 1989 to 2018 (the black solid circle: the local type, the red solid circle: the eastward type, the blue solid circle: the northeastward type, the green solid circle: the southward type, different sizes of solid circles indicate different frequencies of occurrence)

    图  2  1989~2018年6~8月(a)源地型、(b)偏东型、(c)东北型和(d)偏南型九龙涡生成前12 h的整层水汽通量(矢量,单位:kg m−1 s−1)、水汽通量散度(填色,单位:g m−2 s−1)分布。虚线矩形框为九龙涡生成区

    Figure  2.  Distributions of the entire level of water vapor flux (vectors, units: kg m−1 s−1) and water vapor flux divergence (coloring, units: g m−2 s−1) of the (a) local, (b) eastward, (c) northeastward, and (d) southward JLV 12 h before formation during June–August from 1989 to 2018. The dotted rectangular frame indicates the generating area of the JLV

    图  3  1989~2018年6~8月(a)源地型、(b)偏东型、(c)东北型和(d)偏南型九龙涡结束时次的整层水汽通量(矢量,单位:kg m−1 s−1)、水汽通量散度(填色,单位:g m−2 s−1)分布。虚线矩形框为九龙涡生成区,红色打点处表示与源地型相比通过了90%显著性检验的水汽通量散度负异常区域

    Figure  3.  Distributions of the entire level of water vapor flux (vectors, units: kg m−1 s−1) and water vapor flux divergence (coloring, units: g m−2 s−1) of the (a) local, (b) eastward, (c) northeastward, and (d) southward JLV at the end time during June–August from 1989 to 2018. The dotted rectangular frame represents the generating area of JLV, and the red dots show the negative anomaly area of water vapor flux divergence that has passed the 90% significance test compared with the local type

    图  4  1989~2018年6~8月子区域1(第一行)、子区域2(第二行)的源地型(线形A)、偏东型(线形B)、东北型(线形C)、偏南型(线形D)九龙涡初生时次涡区平均热量收支[单位:K (6 h)−1]及其分量的合成垂直分布:(a、e)$ \partial T/\partial t $;(b、f)$-{\boldsymbol{V}}\cdot \nabla T$;(c、g)$ -{\left(p/{p}_{0}\right)}^{\kappa }\omega \partial \theta /\partial p $;(d、h)$ {Q}_{1}{/c}_{p} $

    Figure  4.  Composite vertical distribution of the average heat budget [units: K (6 h)−1] and its components in the main area of the vortex at the time of birth of the local (line A), eastward (line B), northeastward (line C), and southward (line D) JLV in subregion 1 (top line) and subregion 2 (bottom line) during June–August from 1989 to 2018: (a, e) $ \partial T/\partial t $; (b, f) $-{\boldsymbol{V}}\cdot \nabla T$; (c, g)$ -{\left(p/{p}_{0}\right)}^{\kappa }\omega \partial \theta /\partial p $; (d, h) $ {Q}_{1}{/c}_{p} $

    图  5  1989~2018年6~8月子区域1(第一行)、子区域2(第二行)的源地型(线形A)、偏东型(线形B)、东北型(线形C)、偏南型(线形D)九龙涡初生时次涡区平均水汽收支[单位:g kg−1 (6 h)−1]及其分量的合成垂直分布:(a、e)$ \partial q/\partial t $;(b、f)$-{\boldsymbol{V}}\cdot \nabla q$;(c、g)$ -\omega \partial q/\partial p $;(d、h)$ -{Q}_{2}/L $

    Figure  5.  Composite vertical distributions of the average water vapor budget [units: g kg−1 (6 h)−1] and its components in the main area of the vortex at the time of birth of the local (line A), eastward (line B), northeastward (line C), and southward (Line D) JLV in subregion 1 (top line) and subregion 2 (bottom line) during June–August from 1989 to 2018: (a, e) $ \partial q/\partial t $; (b, f) $-{\boldsymbol{V}}\cdot \nabla q$; (c, g) $ -\omega \partial q/\partial p $; (d, h) $ -{Q}_{2}/L $

    图  6  1989~2018年6~8月子区域1的(a、e)源地型、(b、f)偏东型、(c、g)东北型和(d、h)偏南型九龙涡初生时次(第一行)、结束时次(第二行)整层Q1(填色)、Q2(等值线)的合成分布,单位:W m−2。坐标(0, 0)为九龙涡合成中心

    Figure  6.  Composite distributions of the entire level of Q1 (coloring) and Q2 (contours) at the birth time (top line) and the end time (bottom line) of the (a, e) local, (b, f) eastward, (c, g) northeastward, and (d, h) southward JLV in subregion 1 during June–August from 1989 to 2018, units: W m−2. The coordinates (0, 0) represent the composite center of the JLV

    图  7  1989~2018年6~8月子区域2的(a、d)源地型、(b、e)偏东型和(c、f)东北型九龙涡初生时次(第一行)、结束时次(第二行)整层Q1(填色)、Q2(等值线)的合成分布,单位:W m−2。坐标(0, 0)为九龙涡合成中心

    Figure  7.  Composite distributions of the entire level of Q1 (coloring) and Q2 (contours) at the birth time (top line) and the end time (bottom line) of the (a, d) local, (b, e) eastward, and (c, f) northeastward JLV in subregion 2 during June–August from 1989 to 2018, units: W m−2. The coordinates (0, 0) represent the composite center of the JLV

    表  1  1989~2018年6~8月子区域1、子区域2各类九龙涡涡区Q1Q2的平均值和极大值

    Table  1.   Average and extreme values of Q1 and Q2 of various types of JLV in subregions 1 and 2 during June–August from 1989 to 2018

    区域类型Q1最大值/W m−2Q2最大值/W m−2Q1平均值/W m−2Q1平均值/W m−2
    初生时次结束时次初生时次结束时次初生时次结束时次初生时次结束时次
    子区域1源地型659.7748.9(+)848.0866.5(+)192.8242.4(+)310.8261.9(-)
    偏东型541.0772.2(+)677.7811.2(+)183.7403.9(+)243.8406.5(+)
    东北型1384.21878.6(+)1513.92070.3(+)493.3539.9(+)543.4599.0(+)
    偏南型1202.61565.2(+)1407.81573.4(+)548.7543.8(-)580.1588.1(+)
    子区域2源地型945.11164.1(+)1225.91288.1(+)350.1343.8(-)381.7367.2(-)
    偏东型949.11113.5(+)1113.41311.7(+)424.1364.0(-)357.9391.3(+)
    东北型1111.01664.0(+)1451.11601.6(+)374.2503.6(+)400.2457.8(+)
    注:表中的(+)和(-)代表结束时次该物理量比初生时次大、小。
    下载: 导出CSV
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出版历程
  • 收稿日期:  2021-11-02
  • 录用日期:  2022-11-15
  • 网络出版日期:  2023-01-06
  • 刊出日期:  2023-09-27

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