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CN112558188B - A method for improving severe convection forecasting by assimilating lightning data - Google Patents

A method for improving severe convection forecasting by assimilating lightning data Download PDF

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CN112558188B
CN112558188B CN202110089247.5A CN202110089247A CN112558188B CN 112558188 B CN112558188 B CN 112558188B CN 202110089247 A CN202110089247 A CN 202110089247A CN 112558188 B CN112558188 B CN 112558188B
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甘茹蕙
杨毅
郭树昌
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Lanzhou University
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Abstract

The invention relates to a method for improving strong convection forecast by assimilating lightning data, which comprises the following steps: establishing an observation operator between lightning frequency and maximum vertical speed; extracting lightning data 20 minutes before the assimilation moment, converting the lightning data into the maximum vertical speed on a grid of 1 km, and distributing the maximum vertical speed of 1 km to a numerical mode grid; thirdly, according to the GGF method, calculating by using a background field to obtain a vertical localization function of each variable; fourthly, assimilating the maximum vertical speed of the agent by using an ensemble root mean square filtering method and combining a vertical localization function, and circularly assimilating for four times to obtain an analysis field; fifthly, continuously forecasting by utilizing the analysis field to obtain a forecasting field; sixthly, performing forecast inspection. The method effectively improves the dynamic field in the background field by assimilating total flash data, also improves the humidity field and the temperature field to a certain extent, is reasonable and effective, and obviously improves the forecast effect of rainfall and echo waves in a numerical mode.

Description

一种通过同化闪电资料改进强对流预报的方法A method for improving severe convection forecasting by assimilating lightning data

技术领域technical field

本发明涉及气象数据处理方法,尤其涉及一种通过同化闪电资料改进强对流预报的方法。The invention relates to a meteorological data processing method, in particular to a method for improving strong convection forecast by assimilating lightning data.

背景技术Background technique

尽管天气预报不断改进,但由于这些事件涉及的尺度和物理过程的多样性,实现对流活动预警的准确性仍然是一个很大的挑战。强对流天气通常伴有频繁的闪电活动,闪电可用于监测中尺度对流活动的发生和发展,闪电资料同化也是一种非常有用的方法,可以提高初始条件的准确性,从而改善天气预报。Despite continuous improvements in weather forecasting, achieving the accuracy of early warnings of convective activity remains a great challenge due to the diversity of scales and physical processes involved in these events. Strong convective weather is usually accompanied by frequent lightning activities. Lightning can be used to monitor the occurrence and development of mesoscale convective activities. Lightning data assimilation is also a very useful method to improve the accuracy of initial conditions and thus improve weather forecasting.

Browning(1989)提出调整中尺度数值天气预报模式初始场的一种可能方法是改进水汽分析,目前许多闪电资料同化研究都是通过改善初始条件下的水汽场进而改进预报。Alexander等(1999)基于降雨率和闪电之间的关系实现了闪电资料的同化。Fierro等(2012)提出可以通过改变混合区(0°C和-20°C)的水汽混合比例来同化对流分辨尺度下的闪电资料。自此之后,基于Fierro的方法开展了很多闪电资料同化的工作,结果表明:无论是采用不同的同化方法同化代理水汽混合比,或者是基于不同的模式同化代理水汽混合比都可以改善预报。Browning (1989) proposed that a possible method to adjust the initial field of the mesoscale numerical weather prediction model is to improve the water vapor analysis. At present, many lightning data assimilation studies are to improve the forecast by improving the water vapor field under the initial conditions. (1999) realized the assimilation of lightning data based on the relationship between rainfall rate and lightning. (2012) proposed that lightning data at the convective-resolved scale can be assimilated by changing the water-vapor mixing ratio in the mixing region (0°C and -20°C). Since then, a lot of lightning data assimilation work has been carried out based on Fierro's method. The results show that the forecast can be improved whether using different assimilation methods to assimilate the proxy water vapor mixing ratio, or assimilating the proxy water vapor mixing ratio based on different models.

此外,Qie等(2014)建立了总闪电率与冰相粒子(霰、冰、雪)混合比之间的经验公式,用以调整混合区冰相粒子的混合比例。Chen 等(2018)利用Fierro和Qie的方法,利用闪电资料同时调整了混合区低层水汽量和霰质量,并且考虑了模型网格内的热力学和动力学条件,维持模型平衡。此外,Allen等(2016)和Kong等(2020)也利用闪电和霰质量、霰体积之间的观测算子同化了闪电资料。In addition, Qie et al. (2014) established an empirical formula between the total lightning rate and the mixing ratio of ice-phase particles (graupel, ice, and snow) to adjust the mixing ratio of ice-phase particles in the mixing zone. Chen et al. (2018) used the method of Fierro and Qie to simultaneously adjust the low-level water vapor and graupel mass in the mixing zone using lightning data, and considered the thermodynamic and kinetic conditions in the model grid to maintain the model balance. In addition, Allen et al. (2016) and Kong et al. (2020) also assimilated lightning data using the observation operator between lightning and graupel mass and graupel volume.

调整数值模式初始场中的垂直速度分布是改善强对流预报的另一种可行的方法。目前的研究多集中在水汽和水物质的同化上,考虑同化风场特别是垂直速度的研究较少。已有研究表明,上升气流强度与观测到的闪电频数有定性的相关性(Deierling和Petersen, 2008)。根据闪电观测结果,Williams和Earl(1985)表明,陆地对流过程中的总闪频率与对流云高度有大约五次方关系。Price和Rind(1992)指出,根据许多对流事件,对流云中的最大上升速度与云高相关,他们分别建立了大陆云和海洋云中最大垂直速度和总闪频率的经验公式。Wang等(2020b)根据Price和Rind的公式,采用Nudging方法同化闪电数据,调整动态场。此外,很少有研究旨在基于闪电和上升气流的关系来优化动态场。Adjusting the vertical velocity distribution in the initial field of a numerical model is another feasible method to improve severe convection forecasts. At present, most of the researches focus on the assimilation of water vapor and water substances, and few studies consider the assimilation wind field, especially the vertical velocity. Previous studies have shown that there is a qualitative correlation between updraft strength and observed lightning frequency (Deierling and Petersen, 2008). Based on lightning observations, Williams and Earl (1985) showed that the total flash frequency during terrestrial convection has an approximately fifth power relationship with the height of convective clouds. Price and Rind (1992) pointed out that from many convective events, the maximum ascent velocity in convective clouds is related to cloud height, and they established empirical formulas for the maximum vertical velocity and total flash frequency in continental and oceanic clouds, respectively. (2020b) adopted the Nudging method to assimilate the lightning data and adjusted the dynamic field according to the formula of Price and Rind. Furthermore, few studies have aimed to optimize dynamic fields based on the relationship between lightning and updrafts.

集合均方根滤波(EnSRF)使用预测的集合来估计流依赖的背景误差协方差,它已被用于同化常规观测、雷达、卫星和闪电数据(Gao和Min,2018;Wang等,2015)。局地化(Anderson,2007b;Hamill等人,2001)和协方差膨胀(Anderson,2007a,2008)对于EnSRF来说是必不可少的,因为它们会受到小集合数导致的采样误差的影响(Lei和Anderson,2014)。常用的局地化函数是一个近似高斯的五阶多项式函数(Gaspari和Cohn,1999,简称GC函数),GC的宽度参数需要针对给定的情况进行调整,这对于各种观测和状态变量来说是不实用的。此外,还有一些关于自适应协方差的理论研究(Anderson和Lei,2013;Lei等,2014;Lei和Anderson,2014),但关于二维变量最大垂直速度、垂直局地化的概念并没有很好的定义。Lei等(2016)提出了一种GGF(global group filter)方法,可以提供垂直局地化函数的自适应估计,随后,GGF定位函数被应用于ANSU-A辐射数据同化中,获得了较好的预报效果(Lei等,2016;Wang等,2020a)。Ensemble root mean square filtering (EnSRF) uses the predicted ensemble to estimate flow-dependent background error covariance, and it has been used to assimilate conventional observation, radar, satellite, and lightning data (Gao and Min, 2018; Wang et al., 2015). Localization (Anderson, 2007b; Hamill et al., 2001) and covariance inflation (Anderson, 2007a, 2008) are essential for EnSRF because they suffer from sampling errors due to small set numbers (Lei and Anderson, 2014). The commonly used localization function is an approximate Gaussian fifth-order polynomial function (Gaspari and Cohn, 1999, referred to as GC function), and the width parameter of GC needs to be adjusted for a given situation, which is for various observations and state variables. is not practical. In addition, there are some theoretical studies on adaptive covariance (Anderson and Lei, 2013; Lei et al., 2014; Lei and Anderson, 2014), but the concepts of maximum vertical velocity, vertical localization of two-dimensional variables are not very good definition. Lei et al. (2016) proposed a GGF (global group filter) method, which can provide an adaptive estimation of the vertical localization function. Subsequently, the GGF localization function was applied to the ANSU-A radiation data assimilation and obtained better results. forecast effect (Lei et al., 2016; Wang et al., 2020a).

本发明基于2019年7月6日发生的强对流事件,根据总闪和最大垂直速度之间的“瞬时”关系,使用EnSRF方法以及GGF局地化方法同化由总闪数据转换的最大垂直速度(EnSRF_Wmax),以期改善强对流过程的预报。Based on the strong convective event that occurred on July 6, 2019, the present invention uses the EnSRF method as well as the GGF localization method to assimilate the maximum vertical velocity ( EnSRF_Wmax), in order to improve the forecast of strong convective processes.

发明内容SUMMARY OF THE INVENTION

本发明所要解决的技术问题是提供一种合理有效的通过同化闪电资料改进强对流预报的方法。The technical problem to be solved by the present invention is to provide a reasonable and effective method for improving strong convection forecast by assimilating lightning data.

为解决上述问题,本发明所述的一种通过同化闪电资料改进强对流预报的方法,包括以下步骤:In order to solve the above problems, a method for improving strong convection forecasting by assimilating lightning data according to the present invention includes the following steps:

⑴根据对流活动中闪电频数和云顶高度之间的关系为:

Figure 100002_DEST_PATH_IMAGE001
,而最大垂直速度与云顶高度之间的关系为
Figure 868751DEST_PATH_IMAGE002
,建立闪电频数和最大垂直速度之间的观测算子:
Figure 100002_DEST_PATH_IMAGE003
;(1) According to the relationship between lightning frequency and cloud top height in convective activity:
Figure 100002_DEST_PATH_IMAGE001
, while the relationship between maximum vertical velocity and cloud top height is
Figure 868751DEST_PATH_IMAGE002
, establish the observation operator between the lightning frequency and the maximum vertical velocity:
Figure 100002_DEST_PATH_IMAGE003
;

式中:w max 表示最大垂直速度,单位:m/s;F为每公里每分钟的闪电频数; Z为云顶高度,单位:km;In the formula: w max represents the maximum vertical speed, unit: m/s; F is the lightning frequency per kilometer per minute; Z is the height of cloud top, unit: km;

⑵提取同化时刻前20分钟的闪电资料,根据所述闪电频数和最大垂直速度之间的观测算子将所述闪电资料转化为1 km的网格上的最大垂直速度,然后将该1 km的最大垂直速度分配到数值模式网格上;(2) Extract the lightning data 20 minutes before the assimilation time, convert the lightning data into the maximum vertical speed on a 1 km grid according to the observation operator between the lightning frequency and the maximum vertical speed, and then convert the 1 km The maximum vertical speed is assigned to the numerical mode grid;

⑶根据GGF方法,利用背景场计算得到各个变量的垂直局地化函数;(3) According to the GGF method, the vertical localization function of each variable is obtained by using the background field calculation;

⑷利用集合均方根滤波方法,结合所述垂直局地化函数同化代理最大垂直速度,循环同化四次后得到分析场;(4) Using the ensemble root mean square filtering method, combined with the vertical localization function to assimilate the maximum vertical velocity of the agent, and obtain the analysis field after cyclic assimilation four times;

⑸利用所述分析场继续预报得到预报场;(5) Use the analysis field to continue forecasting to obtain the forecast field;

⑹进行预报检验。⑹ Carry out forecast inspection.

所述步骤⑶中垂直局地化函数按下述方法计算:In the described step (3), the vertical localization function is calculated as follows:

①令N表示样本大小,L表示观测数,M表示模式的垂直层,

Figure 822102DEST_PATH_IMAGE004
表示来自第n个样本的第m层的第l个观测处的模式状态变量;其中
Figure 100002_DEST_PATH_IMAGE005
Figure 575163DEST_PATH_IMAGE006
Figure 100002_DEST_PATH_IMAGE007
Figure 814515DEST_PATH_IMAGE008
Figure 362040DEST_PATH_IMAGE004
的集合平均;① Let N denote the sample size, L denote the number of observations, and M denote the vertical layer of the pattern,
Figure 822102DEST_PATH_IMAGE004
represents the mode state variable at the lth observation from the mth layer of the nth sample; where
Figure 100002_DEST_PATH_IMAGE005
,
Figure 575163DEST_PATH_IMAGE006
,
Figure 100002_DEST_PATH_IMAGE007
;
Figure 814515DEST_PATH_IMAGE008
Yes
Figure 362040DEST_PATH_IMAGE004
the ensemble average of ;

②按下述方法根据背景场构造一组观测扰动:

Figure 100002_DEST_PATH_IMAGE009
Figure 686842DEST_PATH_IMAGE010
;式中:
Figure 100002_DEST_PATH_IMAGE011
代表来自第n个样本的第l个观测;
Figure 243594DEST_PATH_IMAGE012
是由闪电转换的第l个最大垂直速度;
Figure 100002_DEST_PATH_IMAGE013
是计算得到的第n个样本的观测扰动;
Figure 71873DEST_PATH_IMAGE014
Figure 100002_DEST_PATH_IMAGE015
的平均,其中
Figure 58808DEST_PATH_IMAGE015
Figure 667644DEST_PATH_IMAGE016
的平均,
Figure 100002_DEST_PATH_IMAGE017
Figure 778819DEST_PATH_IMAGE018
是观测算子;②Construct a set of observation disturbances according to the background field according to the following methods:
Figure 100002_DEST_PATH_IMAGE009
,
Figure 686842DEST_PATH_IMAGE010
; where:
Figure 100002_DEST_PATH_IMAGE011
represents the lth observation from the nth sample;
Figure 243594DEST_PATH_IMAGE012
is the l -th maximum vertical velocity converted by lightning;
Figure 100002_DEST_PATH_IMAGE013
is the calculated observed disturbance of the nth sample;
Figure 71873DEST_PATH_IMAGE014
Yes
Figure 100002_DEST_PATH_IMAGE015
the average of which
Figure 58808DEST_PATH_IMAGE015
Yes
Figure 667644DEST_PATH_IMAGE016
Average,
Figure 100002_DEST_PATH_IMAGE017
,
Figure 778819DEST_PATH_IMAGE018
is the observation operator;

③观测和模式变量之间的相关系数可以通过以下公式计算:③ The correlation coefficient between observations and model variables can be calculated by the following formula:

Figure 100002_DEST_PATH_IMAGE019
Figure 100002_DEST_PATH_IMAGE019
;

式中:

Figure 976451DEST_PATH_IMAGE020
为相关系数;
Figure 100002_DEST_PATH_IMAGE021
代表
Figure 882090DEST_PATH_IMAGE022
的集合平均;where:
Figure 976451DEST_PATH_IMAGE020
is the correlation coefficient;
Figure 100002_DEST_PATH_IMAGE021
represent
Figure 882090DEST_PATH_IMAGE022
the ensemble average of ;

④相关系数

Figure 165173DEST_PATH_IMAGE020
随机地分为G个组,每个组有Q个样本,则相关系数
Figure 876777DEST_PATH_IMAGE020
表示为
Figure 100002_DEST_PATH_IMAGE023
Figure 679648DEST_PATH_IMAGE024
以及
Figure 100002_DEST_PATH_IMAGE025
,所有的G个组中Q个样本的估计相关的均方根(RMS)差
Figure 5456DEST_PATH_IMAGE026
表示为:④Correlation coefficient
Figure 165173DEST_PATH_IMAGE020
Randomly divided into G groups, each group has Q samples, then the correlation coefficient
Figure 876777DEST_PATH_IMAGE020
Expressed as
Figure 100002_DEST_PATH_IMAGE023
,
Figure 679648DEST_PATH_IMAGE024
as well as
Figure 100002_DEST_PATH_IMAGE025
, the estimated correlated root mean square (RMS) difference of Q samples in all G groups
Figure 5456DEST_PATH_IMAGE026
Expressed as:

Figure 100002_DEST_PATH_IMAGE027
Figure 100002_DEST_PATH_IMAGE027
;

均方根最小化得到:

Figure 716447DEST_PATH_IMAGE028
Figure 100002_DEST_PATH_IMAGE029
是计算得到的自适应的垂直局地化函数,即GGF函数; G取16。Root mean square minimization yields:
Figure 716447DEST_PATH_IMAGE028
,
Figure 100002_DEST_PATH_IMAGE029
is the calculated adaptive vertical localization function, namely the GGF function; G takes 16.

所述步骤⑷集合均方根滤波(EnSRF)方法中的观测变量是最大垂直速度w max ;分析变量包括风场(u,v,w)、扰动位温(prt)、扰动位势(ph)、水汽混合比(qv)、雨水混合比(qr)、冰混合比(qi)、霰混合比(qg)、云混合比(qc)、雪混合比(qs)。The observed variable in the ensemble root mean square filtering (EnSRF) method in the step (4) is the maximum vertical velocity w max ; the analysis variables include wind field ( u, v, w ), perturbation potential temperature ( prt ), perturbation potential ( ph ) , water vapor mixing ratio ( qv ), rainwater mixing ratio ( qr ), ice mixing ratio ( qi ), graupel mixing ratio ( qg ), cloud mixing ratio ( qc ), snow mixing ratio ( qs ).

本发明与现有技术相比具有以下优点:Compared with the prior art, the present invention has the following advantages:

1、本发明基于中尺度数值模式WRF,通过同化闪电资料来改进背景场动力信息的方法(简称EnSRF_Wmax),建立了总闪和最大垂直速度之间的观测算子,利用EnSRF方法同化由闪电资料转换的代理最大垂直速度,并采用GGF垂直局地化方案,有效改进了背景场中的动力信息,不但方法合理有效,而且同时对于背景场中的水汽场、温度场也有一定的调整,进而有效地改进了数值模式对于对流过程中的降水和回波的预报。1. Based on the mesoscale numerical model WRF, the present invention improves the background field dynamic information by assimilating lightning data (referred to as EnSRF_Wmax), establishes an observation operator between the total flash and the maximum vertical velocity, and uses the EnSRF method to assimilate the data from the lightning data. The proxy maximum vertical velocity of the conversion, and the GGF vertical localization scheme is used to effectively improve the dynamic information in the background field. Not only is the method reasonable and effective, but also the water vapor field and temperature field in the background field are adjusted to a certain extent, which is effective Numerical model predictions of precipitation and echoes during convective processes have been significantly improved.

2、相比于同化三维资料,本发明同化二维的最大垂直速度减小了计算量。2. Compared with the assimilation of three-dimensional data, the maximum vertical velocity of the two-dimensional assimilation of the present invention reduces the amount of calculation.

附图说明Description of drawings

下面结合附图对本发明的具体实施方式作进一步详细的说明。The specific embodiments of the present invention will be described in further detail below with reference to the accompanying drawings.

图1为本发明中依据GGF垂直局地化方案计算的模式基本状态量的垂直局地化函数图。其中:(u)、(v)、(w)、(prt)、(ph)、(qv)、(qr)、(qc)、(qg)、(qi)、(qs)分别表示u分量风、v分量风、垂直速度、扰动位温、扰动位势、水汽混合比、雨水混合比、云水混合比、霰混合比、冰混合比、雪混合比。FIG. 1 is a vertical localization function diagram of the mode basic state quantity calculated according to the GGF vertical localization scheme in the present invention. Among them: (u), (v), (w), (prt), (ph), (qv), (qr), (qc), (qg), (qi), (qs) represent the u component wind, respectively , v component wind, vertical velocity, disturbance potential temperature, disturbance potential, water vapor mixing ratio, rain mixing ratio, cloud water mixing ratio, graupel mixing ratio, ice mixing ratio, snow mixing ratio.

图2为本发明中闪电转换为模式网格上的最大垂直速度的示意图。其中:(a)是观测到的20 min内地总闪;(b)是将闪电分配到1 km的网格上的闪电频数;(c)是在1 km网格上将闪电频数转换为最大垂直速度;(d)是将1 km网格上的最大垂直速度分配到模式模拟网格(3 km)。FIG. 2 is a schematic diagram of the conversion of lightning into the maximum vertical velocity on the pattern grid in the present invention. where: (a) is the observed total flash within 20 min; (b) is the lightning frequency assigned to the 1 km grid; (c) is the conversion of the lightning frequency to the maximum vertical on the 1 km grid Velocity; (d) is the assignment of the maximum vertical velocity on the 1 km grid to the model simulation grid (3 km).

图3为本发明中同化时刻前20 min的闪电分布,以及转换得到的最大垂直速度图。其中:(a1)是2019年7月6日03 UTC前20 min的闪电分布;(b1)是2019年7月6日04 UTC前20min的闪电分布;(c1)是2019年7月6日05 UTC前20 min的闪电分布;(d1)是2019年7月6日06UTC前20 min的闪电分布;(a2)是根据闪电频数转换的2019年7月6日03 UTC的最大垂直速度;(b2)是根据闪电频数转换的2019年7月6日04 UTC的最大垂直速度;(c2)是根据闪电频数转换的2019年7月6日05 UTC的最大垂直速度;(d2)是根据闪电频数转换的2019年7月6日06 UTC的最大垂直速度。Figure 3 is the lightning distribution 20 minutes before the assimilation time in the present invention, and the maximum vertical velocity map obtained by conversion. Among them: (a1) is the lightning distribution 20 minutes before 03 UTC on July 6, 2019; (b1) is the lightning distribution 20 minutes before 04 UTC on July 6, 2019; (c1) is July 6, 2019 05 Lightning distribution 20 minutes before UTC; (d1) is the lightning distribution 20 minutes before 06 UTC on July 6, 2019; (a2) is the maximum vertical velocity at 03 UTC on July 6, 2019 converted according to lightning frequency; (b2 ) is the maximum vertical speed on July 6, 2019 04 UTC converted according to the lightning frequency; (c2) is the maximum vertical speed on July 6, 2019 05 UTC converted according to the lightning frequency; (d2) is the maximum vertical speed converted according to the lightning frequency The maximum vertical velocity at 06 UTC on July 6, 2019.

图4为本发明中观测模拟的累积降水分布图。其中:(a1)是观测的2019年7月6日06UTC至09 UTC的累积降水;(a2)是控制实验(CTL)模拟的2019年7月6日06 UTC至09 UTC的累积降水;(a3)是同化试验(LDA_GGF)模拟的2019年7月6日06 UTC至09 UTC的累积降水;(b1)是观测的2019年7月6日09 UTC至12 UTC的累积降水;(b2)是控制实验(CTL)模拟的2019年7月6日09 UTC至12 UTC的累积降水;(b3)是同化试验(LDA_GGF)模拟的2019年7月6日09 UTC至12 UTC的累积降水。Fig. 4 is a distribution diagram of cumulative precipitation observed and simulated in the present invention. Where: (a1) is the observed cumulative precipitation from 06 UTC to 09 UTC on July 6, 2019; (a2) is the cumulative precipitation simulated by the control experiment (CTL) from 06 UTC to 09 UTC on July 6, 2019; (a3 ) is the cumulative precipitation from 06 UTC to 09 UTC on July 6, 2019 simulated by the assimilation experiment (LDA_GGF); (b1) is the observed cumulative precipitation from 09 UTC to 12 UTC on July 6, 2019; (b2) is the control The experimental (CTL) simulated cumulative precipitation from 09 UTC to 12 UTC on July 6, 2019; (b3) is the simulated cumulative precipitation from the assimilation experiment (LDA_GGF) from 09 UTC to 12 UTC on July 6, 2019.

图5为本发明中降水预报性能图。其中:(a)是阈值取1 mm时降水预报的性能图;(b)是阈值取5 mm时降水预报的性能图。FIG. 5 is a performance diagram of precipitation forecasting in the present invention. Among them: (a) is the performance map of precipitation forecast when the threshold is 1 mm; (b) is the performance map of precipitation forecast when the threshold is 5 mm.

具体实施方式Detailed ways

一种通过同化闪电资料改进强对流预报的方法,包括以下步骤:A method for improving severe convective forecasting by assimilating lightning data, comprising the following steps:

⑴由于闪电的观测资料(频数)不是数值模式的模式变量,对其进行同化时首先要建立闪电和其他模式变量的观测算子。(1) Since the observation data (frequency) of lightning is not the model variable of the numerical model, the observation operator of lightning and other model variables must be established first when assimilating it.

已有的研究表明对流活动中闪电频数和云顶高度之间存在五次幂的关系,Ushio等(2001)利用TRMM卫星上降水雷达和闪电成像仪的数据,获得了“瞬时”闪电频数和对流云云顶高度之间的关系为

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,而最大垂直速度与云顶高度之间的关系为
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,因此,建立闪电频数和最大垂直速度之间的观测算子:
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;Existing studies have shown that there is a fifth-power relationship between lightning frequency and cloud top height in convective activity. Ushio et al. (2001) used the data of the precipitation radar and lightning imager on the TRMM satellite to obtain the "instantaneous" lightning frequency and convective cloud cloud. The relationship between the top heights is
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, while the relationship between maximum vertical velocity and cloud top height is
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, therefore, establish the observation operator between the lightning frequency and the maximum vertical velocity:
Figure 323512DEST_PATH_IMAGE003
;

式中:w max 表示最大垂直速度,单位:m/s;F为每公里每分钟的闪电频数;Z为云顶高度,单位:km。Where: w max represents the maximum vertical speed, unit: m/s; F is the lightning frequency per kilometer per minute; Z is the height of the cloud top, unit: km.

此观测算子仅适用于1 km的网格。This observation operator only works on 1 km grids.

⑵提取同化时刻前20分钟的闪电资料,根据闪电频数和最大垂直速度之间的观测算子将闪电资料转化为1 km的网格上的最大垂直速度,然后将该1 km的最大垂直速度分配到数值模式网格上。(2) Extract the lightning data 20 minutes before the assimilation time, convert the lightning data into the maximum vertical speed on a 1 km grid according to the observation operator between the lightning frequency and the maximum vertical speed, and then assign the maximum vertical speed of 1 km to the maximum vertical speed. onto the numerical mode grid.

具体过程:第一步将闪电资料分配到1 km的网格,第二步根据得到的观测算子将1km的闪电频数转换为最大垂直速度,最后再将最大垂直速度转换为模式网格(3 km),具体过程如图2所示。The specific process: the first step assigns the lightning data to a 1 km grid, the second step converts the 1 km lightning frequency into the maximum vertical velocity according to the obtained observation operator, and finally converts the maximum vertical velocity into a pattern grid (3 km), the specific process is shown in Figure 2.

⑶根据GGF(global group filter)方法,利用背景场计算得到各个变量的垂直局地化函数。利用EnSRF方法同化最大垂直速度难点在于垂直局地化方案的设置,本发明中垂直局地化方案采用GGF方案,GGF局地化方案观测和状态变量的扰动集合,利用样本相关计算得到。(3) According to the GGF (global group filter) method, the vertical localization function of each variable is calculated by using the background field. The difficulty of using the EnSRF method to assimilate the maximum vertical velocity lies in the setting of the vertical localization scheme. In the present invention, the vertical localization scheme adopts the GGF scheme. The GGF localization scheme observes the disturbance set of state variables and uses the sample correlation calculation to obtain.

垂直局地化函数按下述方法计算:The vertical localization function is calculated as follows:

①令N表示样本大小,L表示观测数,M表示模式的垂直层,

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表示来自第n个样本的第m层的第l个观测处的模式状态变量;其中
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的集合平均;① Let N denote the sample size, L denote the number of observations, and M denote the vertical layer of the pattern,
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represents the mode state variable at the lth observation from the mth layer of the nth sample; where
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,
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,
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;
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Yes
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the ensemble average of ;

②在EnSRF中没有观测扰动,为了计算GGF垂直局地化函数,需要按下述方法根据背景场构造一组观测扰动:

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;式中:
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代表来自第n个样本的第l个观测;
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是由闪电转换的第l个最大垂直速度;
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是计算得到的第n个样本的观测扰动;
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的平均,其中
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的平均,
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H'是观测算子;在本研究中H'也就是利用背景场计算最大垂直速度的方法。②There is no observation disturbance in EnSRF. In order to calculate the GGF vertical localization function, it is necessary to construct a set of observation disturbances according to the background field according to the following method:
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,
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; where:
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represents the lth observation from the nth sample;
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is the l -th maximum vertical velocity converted by lightning;
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is the observed disturbance of the calculated nth sample;
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Yes
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the average of which
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Yes
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Average,
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, H' is the observation operator; in this study, H' is the method of calculating the maximum vertical velocity using the background field.

③观测和模式变量之间的相关系数可以通过以下公式计算:③ The correlation coefficient between observations and model variables can be calculated by the following formula:

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;

式中:

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为相关系数;
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代表
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的集合平均;where:
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is the correlation coefficient;
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represent
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the ensemble average of ;

④相关系数

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随机地分为G个组,每个组有Q个样本,则相关系数
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表示为
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以及
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,所有的G个组中Q个样本的估计相关的均方根(RMS)差
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表示为:④Correlation coefficient
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Randomly divided into G groups, each group has Q samples, then the correlation coefficient
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Expressed as
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,
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as well as
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, the estimated correlated root mean square (RMS) difference of Q samples in all G groups
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Expressed as:

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;这里的q,i,j没有实际的意义,就是数组算法的表示,求和算法,q从1取到Q,i从1取到G,j从1取到G,其中j不等于i。
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; The q, i, j here have no practical meaning, they are the representation of the array algorithm, the summation algorithm, q is taken from 1 to Q, i is taken from 1 to G, and j is taken from 1 to G, where j is not equal to i.

均方根最小化得到:

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是计算得到的自适应的垂直局地化函数,即GGF函数; G取16。Root mean square minimization yields:
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,
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is the calculated adaptive vertical localization function, namely the GGF function; G takes 16.

计算得到的模式基本量的局地化函数的归一结果如图1所示。The normalized result of the localization function of the calculated basic quantity of the pattern is shown in Fig. 1.

⑷利用集合均方根滤波(EnSRF)方法,结合垂直局地化函数同化代理最大垂直速度,循环同化四次后得到分析场。(4) Using the Ensemble Root Mean Square Filtering (EnSRF) method, combined with the vertical localization function to assimilate the maximum vertical velocity of the proxy, and obtain the analysis field after cyclic assimilation four times.

由于最大垂直速度是一个特殊的二维的变量,集合均方根滤波方法(EnSRF)易于建立最大垂直速度和其他变量之间建立平衡约束,此外EnSRF方法避免了产生扰动观测时生成的采样误差,所以本发明中选用EnSRF同化闪电转换的最大垂直速度。Since the maximum vertical velocity is a special two-dimensional variable, the ensemble root mean square filtering method (EnSRF) is easy to establish a balance constraint between the maximum vertical velocity and other variables. In addition, the EnSRF method avoids the sampling error generated when the perturbed observation is generated. Therefore, in the present invention, the maximum vertical velocity of EnSRF assimilation lightning conversion is selected.

在EnSRF中,上标abo分别表示分析场、背景场以及观测,x b 是模式预报的背景场,y o 为一系列观测,分析场x a 的最小方差估计根据卡尔曼滤波方程可以表示为:In EnSRF , the superscripts a , b , o represent the analysis field, background field and observation, respectively, x b is the background field predicted by the model, yo is a series of observations, and the minimum variance of the analysis field x a is estimated according to the Kalman filter equation It can be expressed as:

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,

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,

其中:H是观测算子H'的线性化形式,观测算子H'是状态量x到观测y o 之间投影关系,K是卡尔曼增益矩阵,Pb是背景误差协方差矩阵,R是观测误差协方差矩阵,在EnSRF中没有观测扰动(

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),集合平均(
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)和第i个集合的偏差(
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)可以表示为:Where: H is the linearized form of the observation operator H ' , the observation operator H' is the projection relationship between the state quantity x and the observation y o , K is the Kalman gain matrix, P b is the background error covariance matrix, R is the Observation error covariance matrix with no observation perturbation in EnSRF (
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), the ensemble average (
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) and the deviation of the ith set (
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)It can be expressed as:

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,

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;

其中

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称为“简化”卡尔曼增益矩阵,定义如下:in
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is called the "simplified" Kalman gain matrix and is defined as:

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Figure 864530DEST_PATH_IMAGE038

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.

在本发明中,观测变量是最大垂直速度w max ;分析变量包括风场(u,v,w)、扰动位温(prt)、扰动位势(ph)、水汽混合比(qv)、雨水混合比(qr)、冰混合比(qi)、霰混合比(qg)、云混合比(qc)、雪混合比(qs)。In the present invention, the observed variable is the maximum vertical velocity w max ; the analysis variables include wind field ( u,v,w ), disturbance potential temperature ( prt ), disturbance potential ( ph ), water vapor mixing ratio ( qv ), rainwater mixing ratio ( qr ), ice mixing ratio ( qi ), graupel mixing ratio ( qg ), cloud mixing ratio ( qc ), snow mixing ratio ( qs ).

⑸利用分析场继续预报得到预报场。⑸ Use the analysis field to continue forecasting to obtain the forecast field.

⑹进行预报检验。⑹ Carry out forecast inspection.

为了验证本发明对强对流预报的改善效果,选取了2019年7月6日发生在我国山东和江苏地区的一次强对流过程进行个例分析,本次试验总共设计一组控制实验以及一组循环同化试验,详细的试验设计如表1所示:In order to verify the improvement effect of the present invention on the forecast of strong convection, a case analysis of a strong convection process that occurred in Shandong and Jiangsu regions of my country on July 6, 2019 was selected for analysis. A set of control experiments and a set of loops were designed in this experiment. Assimilation test, the detailed test design is shown in Table 1:

表1: 试验设计表Table 1: Experimental Design Table

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Figure 524051DEST_PATH_IMAGE040

表1中spin-up的理解为:因为中小尺度模式的都是由无云初始场开始的,所以开始需要一定的时间产生相应的云水信息,冷启动之后会在一段时间内产生实际的云水信息,但是这几个小时内的预报是不准确的,将这几个小时称为“spin-up”时间。也就是说这段时间的模拟结果是不可靠的,所以分析的时候不对spin-up这期间的结果进行分析。The understanding of spin-up in Table 1 is: because the medium and small scale models are all started from the cloud-free initial field, it takes a certain time to generate the corresponding cloud water information at the beginning, and the actual cloud will be generated within a period of time after the cold start. water information, but forecasts for these hours are inaccurate, referring to these hours as "spin-up" time. That is to say, the simulation results during this period are unreliable, so the results of the spin-up period are not analyzed during the analysis.

在上述试验中,试验Ⅰ(CTL)是控制试验,试验Ⅱ(LDA_GGF)是利用EnSRF方法同化闪电的试验,同化时间是2019年7月6日03、04、05、06 UTC。本研究选用WRF 3.6.1版本,21个全国集合成员预报系统的集合预报被用为WRF模式提供初始场和边界场,为了使样本离散度增强,选用RRTMG和Goddard辐射方案使21个样本变成42个样本,除此之外,选用的参数化方案有Thompson微物理方案、Monin-Obukhov近地层方案、Mellor-Yamada-Janjic TKE行星边界层方案、RUC陆面方案,Tiedtke积云参数化方案(只在D01中使用)。本研究采用两重嵌套网格,D01的水平分辨率为9 km,模式网格为171×151,D02水平分辨率为3 km,模式网格为391×271,垂直方向有50层。In the above experiments, experiment I (CTL) is a control experiment, and experiment II (LDA_GGF) is an experiment using the EnSRF method to assimilate lightning. The assimilation time is July 6, 2019 03, 04, 05, 06 UTC. In this study, WRF 3.6.1 version was selected. The ensemble forecast of 21 national ensemble member forecast systems was used to provide the initial field and boundary field for the WRF model. In order to enhance the sample dispersion, the RRTMG and Goddard radiation schemes were used to make the 21 samples become 42 samples. In addition, the selected parameterization schemes include the Thompson microphysics scheme, the Monin-Obukhov near-surface layer scheme, the Mellor-Yamada-Janjic TKE planetary boundary layer scheme, the RUC land surface scheme, and the Tiedtke cumulus parameterization scheme ( Only used in D01). In this study, two nested grids were used, the horizontal resolution of D01 was 9 km, the model grid was 171×151, and the horizontal resolution of D02 was 3 km, the model grid was 391×271, and there were 50 layers in the vertical direction.

本研究选用EnSRF方案同化最大垂直速度,垂直局地化方案选用的是GGF局地化方案,图1所示是根据GGF局地化方案计算的模式状态量的局地化函数。本研究还建立了最大垂直速度和闪电频数之间的观测算子,图2 是将闪电观测转换为模式网格上最大垂直速度的过程,图3所示是本次试验中用到的闪电资料的分布,图3(a1-d1)是同化时刻整点前20min的累积闪电,图3(a2-d2)是依据建立的观测算子转换得到的最大垂直速度,可以看出这次对流过程发生了很多次闪电过程,03 UTC闪电多集中在山东地区,之后对流过程以较快的速度向南移动,至06 UTC闪电主要分布在江苏的北部。In this study, the EnSRF scheme is used to assimilate the maximum vertical velocity, and the vertical localization scheme is the GGF localization scheme. Figure 1 shows the localization function of the mode state quantity calculated according to the GGF localization scheme. This study also established an observation operator between the maximum vertical velocity and the lightning frequency. Figure 2 shows the process of converting lightning observations to the maximum vertical velocity on the model grid. Figure 3 shows the lightning data used in this experiment. Figure 3 (a1-d1) is the accumulated lightning 20 minutes before the assimilation time on the hour, Figure 3 (a2-d2) is the maximum vertical velocity obtained by the conversion of the established observation operator, it can be seen that this convection process occurred After many lightning processes, the 03 UTC lightning was mostly concentrated in the Shandong area, and then the convective process moved southward at a faster speed, and by 06 UTC the lightning was mainly distributed in the northern part of Jiangsu.

图4是观测和模拟的累积降水分布,第一行是2019年7月6如06-09 UTC的累积降水,第二行是09-12 UTC的累积降水,第一列是观测降水,第二列是控制实验模拟的降水,第三列是同化试验模拟的降水,06-09 UTC观测降水主要集中在江苏北部,控制实验没有模拟出江苏地区主要的雨带,而同化试验较好地改进了江苏地区的降水,09-12 UTC观测的降水主要集中在江苏的南部,而模拟的降水位置偏北,同化试验模拟的雨带和观测的雨带位置比较接近。Figure 4 is the distribution of the observed and simulated cumulative precipitation, the first row is the cumulative precipitation from 06-09 UTC on July 6, 2019, the second row is the cumulative precipitation from 09-12 UTC, the first column is the observed precipitation, the second The column is the precipitation simulated by the control experiment, and the third column is the precipitation simulated by the assimilation experiment. The observed precipitation from 06-09 UTC is mainly concentrated in northern Jiangsu. The control experiment did not simulate the main rainbands in Jiangsu, while the assimilation experiment improved well. For the precipitation in Jiangsu, the precipitation observed from 09-12 UTC is mainly concentrated in the southern part of Jiangsu, while the simulated precipitation is located in the north.

图5是降水预报性能图,图(a)和图(b)分别表示选取1 mm、5 mm阈值的结果,预报性能图可以反映很多信息,包括预报偏差(FR,图中虚线所示,越接近1表明预报偏差越小,大于1表示高估,小于1表示低估)、命中率(POD,越高表明预报越好)、临界成功指数(CSI,图中曲线所示,范围0-1,约接近于1越好)、成功率(SR,1减去空报率,越接近于1越好),综合来说在预报性能图中约接近于右上角,表明预报效果越准确。图中浅色圆圈表示控制试验结果,深色表示同化试验结果,可以看出对于较小的阈值,同化试验在6小时预报都显著优于控制实验,当阈值取5 mm时,同化试验在前4个小时的预报效果较好。总体来看同化试验预报效果显著优于控制试验。Figure 5 is the precipitation forecast performance map. Figures (a) and (b) represent the results of selecting 1 mm and 5 mm thresholds, respectively. The forecast performance map can reflect a lot of information, including the forecast deviation (FR, shown by the dotted line in the figure, the more Close to 1 indicates that the forecast deviation is smaller, greater than 1 indicates overestimation, and less than 1 indicates underestimation), hit rate (POD, higher indicates better forecast), critical success index (CSI, as shown by the curve in the figure, the range is 0-1, It is close to 1, the better), the success rate (SR, 1 minus the empty alarm rate, the closer it is to 1, the better). Generally speaking, it is close to the upper right corner in the forecast performance graph, indicating that the forecast effect is more accurate. The light circles in the figure represent the results of the control experiment, and the dark circles represent the results of the assimilation experiment. It can be seen that for a smaller threshold, the assimilation experiment is significantly better than the control experiment at 6 hours. When the threshold is 5 mm, the assimilation experiment is in the front. A 4-hour forecast is better. In general, the prediction effect of the assimilation experiment is significantly better than that of the control experiment.

Claims (2)

1. A method for improving strong convection forecasts by assimilating lightning data, comprising the steps of:
the method comprises the following steps of according to the relation between the lightning frequency and the cloud top height in the convection activity:
Figure DEST_PATH_IMAGE001
and the relationship between the maximum vertical velocity and the height of the cloud top is
Figure 232582DEST_PATH_IMAGE002
Establishing an observation operator between the lightning frequency and the maximum vertical speed:
Figure DEST_PATH_IMAGE003
in the formula:w max represents the maximum vertical velocity, in units: m/s; f is the lightning frequency per kilometer per minute; z is the cloud top height in units: km;
secondly, extracting lightning data 20 minutes before the assimilation moment, converting the lightning data into the maximum vertical speed on a1 km grid according to an observation operator between the lightning frequency and the maximum vertical speed, and then distributing the 1 km maximum vertical speed to a numerical mode grid;
thirdly, according to the GGF method, calculating by using a background field to obtain a vertical localization function of each variable; the vertical localization function is calculated as follows:
let N denote the sample size,Lrepresenting the number of observations, M represents the vertical layer of the mode,
Figure 930410DEST_PATH_IMAGE004
is indicated from the firstnA first sample ofmFirst of the layerlMode state variables at each observation; wherein
Figure DEST_PATH_IMAGE005
Figure 72810DEST_PATH_IMAGE006
Figure DEST_PATH_IMAGE007
Figure 161725DEST_PATH_IMAGE008
Is that
Figure 830603DEST_PATH_IMAGE004
(ii) ensemble averaging;
secondly, a group of observation disturbances is constructed according to the background field by the following method:
Figure DEST_PATH_IMAGE009
Figure 699333DEST_PATH_IMAGE010
(ii) a In the formula:
Figure DEST_PATH_IMAGE011
represents from the firstnA first sample ofl(ii) an observation;
Figure 391346DEST_PATH_IMAGE012
is converted by lightninglA maximum vertical velocity;
Figure DEST_PATH_IMAGE013
is calculated to ben(ii) observed perturbations of individual samples;
Figure 879090DEST_PATH_IMAGE014
is that
Figure DEST_PATH_IMAGE015
Wherein, on average
Figure 274912DEST_PATH_IMAGE015
Is that
Figure 642439DEST_PATH_IMAGE016
Is calculated based on the average of (a) and (b),
Figure DEST_PATH_IMAGE017
Figure 821748DEST_PATH_IMAGE018
is an observation operator;
③ the correlation coefficient between the observation and the mode variables can be calculated by the following formula:
Figure DEST_PATH_IMAGE019
in the formula:
Figure 847604DEST_PATH_IMAGE020
is a correlation coefficient;
Figure DEST_PATH_IMAGE021
represents
Figure 244737DEST_PATH_IMAGE022
(ii) ensemble averaging;
correlation coefficient
Figure 579903DEST_PATH_IMAGE020
Is randomly divided intoGGroups, each group havingQSample by sample, correlation coefficient
Figure 246508DEST_PATH_IMAGE020
Is shown as
Figure DEST_PATH_IMAGE023
Figure 263005DEST_PATH_IMAGE024
And
Figure DEST_PATH_IMAGE025
all ofGIn a groupQRoot mean square deviation of estimated correlations of individual samples
Figure 636349DEST_PATH_IMAGE026
Expressed as:
Figure DEST_PATH_IMAGE027
root mean square minimization yields:
Figure 342749DEST_PATH_IMAGE028
Figure DEST_PATH_IMAGE029
is a self-adaptive vertical localization function obtained by calculation, namely a GGF function; Gtaking 16;
fourthly, utilizing an ensemble root mean square filtering method, assimilating the maximum vertical speed of the agent by combining the vertical localization function, and circularly assimilating for four times to obtain an analysis field;
in EnSRF, superscriptaboRespectively representing the analysis field, the background field and the observation,x b is the background field of the mode forecast,y o analyzing the field for a series of observationsx a The minimum variance estimate of (c) can be expressed as:
Figure 168754DEST_PATH_IMAGE030
Figure DEST_PATH_IMAGE031
wherein: h is an observation operatorH'Of the linearized form, observation operatorH'Is a state quantityxTo observey o K is a kalman gain matrix,Pbis the background error covariance matrix, R is the observation error covariance matrix, and there is no observed perturbation in EnSRF: (
Figure 926626DEST_PATH_IMAGE032
) Ensemble averaging (A)
Figure DEST_PATH_IMAGE033
) And a firstiDeviation of a set (
Figure 92159DEST_PATH_IMAGE034
) Can be expressed as:
Figure DEST_PATH_IMAGE035
Figure 963601DEST_PATH_IMAGE036
wherein
Figure DEST_PATH_IMAGE037
Referred to as a "simplified" kalman gain matrix, defined as follows:
Figure 339219DEST_PATH_IMAGE038
Figure DEST_PATH_IMAGE039
fifthly, continuously forecasting by utilizing the analysis field to obtain a forecasting field;
sixthly, forecasting and checking.
2. A method of improving a strong convection forecast by assimilating lightning data according to claim 1, characterized by: fourth step of collecting observation variable in root mean square filtering method as maximum sagStraight speedw max (ii) a The analysis variables include wind field, disturbance potential temperature, disturbance potential, water-vapor mixing ratio, rainwater mixing ratio, ice mixing ratio, aragonite mixing ratio, cloud mixing ratio, snow mixing ratio.
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