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Severe convective weather (SCW), such as short-duration heavy rainfall (SDHR), severe convective winds, and hail, appears frequently in China. Many previous studies focused on the occurrence and development of SCW (Maddox [1]; Tao [2]; Houze Jr [3]; Zhang et al. [4]; Xie et al. [5]; Yu et al. [6]; Zheng et al. [7]). Additionally, it is suggested that SCWs are mostly produced by mesoscale convective systems (MCSs, Maddox [1]; Tollerud and Collander [8]; Doswell [9]; Schumacher and Johnson [10]; Shibagaki et al. [11]). With the advances in satellite remote sensing and radar detection, high spatial and temporal resolution datasets, particularly the stationary satellite observation data with longer time series, higher resolution and better quality control, have been applied to explore the spatial and temporal distribution of MCSs all over the world. (Maddox [1]; Zheng et al. [7]; Augustine and Howard [12]; Laing and Fritsch [13]; Anderson and Arritt [14]; Jirak et al. [15]; Goyens et al. [16]; Zhuo et al. [17]). Maddox [1] defined mesoscale convective complexes (MCCs) using infrared satellite data, with the criteria of temperature of black body (TBB) ≤ -32 ℃ and cloud area ≥ 105 km2, and TBB≤ -52 ℃ and cloud area ≥ 5×104 km2. Based on the definition of Maddox [1], Jirak et al. [15] removed the ≤ -32 ℃ size requirement of the satellite classification scheme in Maddox [1] and further divided the MCSs into four morphologies. Although the infrared satellite data were useful for MCSs'identification and tracking, radar imagery can show the development and three-dimensional structure of MCSs in detail, especially the spatial distributions of convective and stratiform development (Zheng et al. [7]; Schumacher and Johnson [10]; Jirak et al. [15]; Parker and Johnson [18]; Meng et al. [19]; Li et al. [20], Chen et al. [21]).
Numerous studies have used radar data to classify the morphologies of MCSs (e.g., Zheng et al. [7]; Jirak et al. [15]; Parker and Johnson [18]; Bluestein and Jain [22]; Blanchard [23]; Loehrer and Johnson [24]; Wang et al. [25]; Yang and Sun [26]). In some earlier studies, severe and non-severe squall lines were documented into four distinct formation modes: broken line, back building, broken area and embedded area (Bluestein and Jain [22]). Parker and Johnson [18] proposed three morphologies for linear convective systems: trailing stratiform precipitation (TS), leading stratiform precipitation (LS) and parallel stratiform precipitation (PS). Based on the above three morphologies of linear convective systems, Gallus Jr et al. [27] classified MCSs into nine morphologies according to the dominant morphology in the radar data, adding individual cells (IC), clusters of cells (CC), broken lines (BL), bow echoes (BE), no stratiform precipitation (NS), and nonlinear systems. It was found that the nine dominant morphologies covered almost all common mesoscale convective storms. Jirak et al. [15] further studied the different patterns of MCSs and classified MCSs into 17 morphologies during the active convective season of the central United States. Some studies examined the organizational modes of MCSs over central east China (Zheng et al. [7]; Wang et al. [25]). Zheng et al. [7] classified the MCSs over central east China into NL and six linear organizational modes: NS, TS, LS, PS, BE, and embedded lines (EL). A statistical analysis of MCSs over Yangtze River Basin found eight morphologies of linear modes: TS, LS, training line/adjoining stratiform, back-building/quasi-stationary MCSs (BB), PS, BL, EL and long line. Yang and Sun [26] collected the severe-wind-producing convective system events over north China and concluded six organizational modes that consist of CC (35.4%), squall lines (18.4%), nonlinear-shaped systems (17.8%), BL (11.6%), IC (1.2%) and BE (0.5%). Recent studies also analyzed the features of MCSs associated with warm-sector heavy rainfall and quasi-linear MCSs in south China. Li et al. [20] examined the organizational modes of mesoscale convective systems (MCSs) associated with warm-sector heavy rainfall events in south China and found that these MCSs can be classified into NL (40%) and eight linear modes (60%): TS, NS, LS, PS, EL, BE, training line/adjoining stratiform, and multiple rain bands (MRB). Chen et al. [21] analyzed the general features and circulation patterns of 98 quasi-linear MCSs over south China, which include TS (39.8%), NS (22.4%), EL(11.2%), PS(10.2%) and multiple convective lines with stratiform precipitation (MLS, 16.3%).
It was shown that different morphologies of MCSs corresponded to different SCWs, such as heavy rainfall, hail, high wind and tornadoes (Zheng et al. [7]; Parker and Johnson [18]; Bluestein and Jain [22]; Yang and Sun [26]; Gallus Jr et al. [27]; Parker [28]; Duda and Gallus Jr [29]; Lombardo and Colle [30]; ). Fujita [31] demonstrated that bow echoes tended to produce more high wind events. Tornadoes were often observed in bow echoes (Trapp et al. [32]) and supercells (Moller et al. [33]). Pettet and Johnson [34] showed that LS and PS squall lines produced more flooding events. It was also found that training line/adjoining stratiform and BB were the two most frequent modes in the 116 extreme rainfall events from 1999 to 2001 in the east of the Rocky Mountains in the United States (Schumacher and Johnson [10]). Duda and Gallus Jr [29] analyzed severe weather reports as a function of convective mode and found substantial differences between the morphologies of severe weather reports and different storm morphologies. Over central east China, BE systems generate the most severe weather on average, while most TS systems are attendant with SDRH and high winds. EL and PS systems are most frequently associated with extreme SDHR (Zheng et al. [7]).
Additionally, the classification of MCSs may be associated with various dynamical and thermal conditions (Zheng et al. [7]; Parker and Johnson [18]; Bluestein and Jain [22]; Yang and Sun [26]; Gallus Jr et al. [27]; Parker [28]; Duda and Gallus Jr [29]; Lombardo and Colle [30]). It has been demonstrated that vertical wind shear is an important factor to distinguish different morphologies of convection systems (Parker and Johnson [18]). It was shown that the type of BE over central east China generally occurs under strong low-level vertical shears. The LS and PS tended to produce flooding events. The physical parameters derived from the environmental soundings of MCSs were compared over different regions between east China and the central United States (Zheng et al. [7]). Precipitable water (PWAT) was another key factor to affect the convection-producing SCWs. It was proposed that PWAT of TS mode is higher than that of LS and PS over the central United States (Parker and Johnson [18]). The high PWAT in moist MCSs over central east China shows great similarity to the results of pre-tropical cyclone (TC) squall lines that occurred over south China (Meng et al. [19]; Meng and Zhang [35]). Zheng et al. [7] also found that severe convective winds and hail events were mainly observed in dry environments (PWAT ≤ 50 mm) and SDHR occurred more frequently in moist environments (PWAT ≥ 50 mm). Different PWAT values correspond to different convection modes, such as 28 mm for convection lines (Bluestein and Jain [22]), 26.9 mm for severe convective windstorms, 33.5 mm for TS mode, 32.7 mm for LS systems, and 24.3 mm for PS type (Parker and Johnson [18]). In addition, thermal environmental conditions were also essential for convection initiation, consisting of surfaced-based convective available potential energy (SBCAPE), lifted index (LI), and lifting condensation level (LCL).
The above recent studies mainly explored the classification features, SCWs and environmental conditions of MCSs in both the east and north China, however, few studies focused on these characteristics of MCSs in south China. It is well known that different synoptic background systems can influence the differences of the organization modes, corresponding SCWs and environmental conditions of MCSs over different regions. The main synoptic systems over south China include a southwesterly low-level jet (LLJ) originated over the tropical oceans, a low-level vortex developing in southwest China and a subtropical high over the northwestern Pacific (WPSH) (Tao and Ding [36]; Ninomiya and Akiyama [37]), which are different with those in both the east and north China. It is essential to explore the general features of MCSs in south China. The goal of this study is to investigate morphologies of MCSs, their corresponding SCWs and the environmental conditions in south China.
Section 2 introduces data and methodology. Morphologies of radar echoes in south China are shown in section 3. Two SCW events corresponding to each morphology mode are compared in section 4. Section 5 analyzes the environmental conditions before convection initiation of different morphologies. Finally, the conclusion is given in section 6.
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Composite Doppler radar reflectivity from April to September of 2011-2015 are used to derive and classify MCSs over south China (18-27°N, 105-120°E, Fig. 1). These composite radar reflectivity data with 10-min temporal and 1 km × 1 km spatial resolutions were provided by the National Meteorological Center (NMC) of the China Meteorological Administration (CMA). Meanwhile, hourly automatic weather station data and 3-hourly severe weather reports are used to analyze severe weather events. According to the definition of NMC, SCW refers to SDHR with hourly precipitation amount ≥ 20 mm h-1, and severe convective winds with speeds higher than or equal to Beaufort scale 8 (or 17.2 m s−1), hail and any tornado, but tornadoes were not considered in this study. The SDHR events are obtained from the automatic weather station data, and severe convective winds and hail events are obtained from severe weather reports. Because of the localization of severe convective winds and hail, these events cannot be fully recorded in automatic weather station data, which report the general occurrence and geographic distribution features of the two SCW events.
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Herein the lifetime of a storm was subjectively determined by the start (end) time of the first (last) radar image where the 30-dBZ contiguous echo coverage exceeded a 30 km x30 km area with a maximum exceeding 45 dBZ for at least 1 h (Zheng et al. [7]). Except for the missing and discontinuous radar mosaic, 1640 reflectivity samples are collected, comprising 208, 267, 251, 459 and 455 samples for 2011, 2012, 2013, 2014 and 2015, respectively (Table 1). Convective and stratiform echoes were defined as those of greater than 40 and 20-40 dBZ, respectively (Parker and Johnson [18]; Geerts [38]). As the pattern of radar echoes varied over the lifetime of a convective system, one individual storm could be classified into different morphologies at its different evolution stages. The classification scheme used in the present study was basically the same as that in G08 except the embedded lines (ELs) as they are a common morphology in China (Zheng et al. [7]; Li et al. [20]; Chen et al. [21]; Wang et al. [25]). The storm morphologies were classified into three types, namely, cellular, linear, and nonlinear systems. The cellular systems were subdivided into individual cells (ICs) and clusters of cells (CCs). ICs were storms without weaker radar echoes (10 dBZ < radar echoes < 40 dBZ) connecting the cells. CCs were storm cells connected by weaker radar echoes. Linear systems were those in which the convective echoes were connected and organized in a linear shape of at least 100 km in length and a length-to-width ratio of at least 3: 1, with these features lasting for at least 1 h. The criteria for linear systems were essentially the same as those in previous studies (Zheng et al. [7]; Chen et al. [21]; Gallus Jr et al. [27]; Yang et al. [39]). The linear systems included six subtypes: trailing stratiform (TSs), leading stratiform (LSs), parallel stratiform (PSs), no stratiform (NSs), bow echoes (BEs) and ELs, which is different from the five organization modes of quasi-linear MCSs, including TSs, NSs, PSs, ELs and MLSs (Chen et al. [21]). A schematic diagram illustrating the classified storm morphologies is given in Fig. 2.
Category 2011 2012 2013 2014 2015 Total IC 17 8 10 9 24 68 CC 60 50 47 136 122 415 TS 8 48 28 34 46 164 PS 2 1 4 5 1 13 LS 0 6 0 2 2 10 BE 1 6 4 6 5 22 EL 12 24 16 18 14 84 NS 9 21 19 32 28 109 NL 99 103 123 217 213 755 Total 208 267 251 459 455 1640 Table 1. Sample distributions of nine storm morphologies.
Figure 2. Schematic illustrations of radar echo morphologies: individual cells (ICs) and clusters of cells (CCs), nonlinear systems (NLs), convective lines with trailing stratiform (TSs), convective lines with leading stratiform (LSs), convective lines with parallel stratiform (PSs), convective lines with no stratiform (NSs), bow echoes (BEs) and embedded lines (Els).
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To explore the environmental conditions associated with various storm morphologies, the environmental physical parameterizations are calculated three hours prior to convection initiation. Because the temporal and spatial resolutions of sounding observation are coarse and most SCWs occur in the afternoon and at night, the sounding observations are too coarse to capture the environment of a SCW event. The thermodynamic soundings are reconstructed using global final-analysis data from National Centers for Environmental Prediction (NCEP FNL, 6-h temporal and 1 °×1 ° spatial resolutions) to create proximity soundings (Lee [40]; Brooks et al. [41]). Considering the large errors between the model near surface level and observations, the surface observation data from automatic weather stations is applied to represent the signals in the lower atmosphere of the reanalysis data (Johnson and Bresch [42]; Pan et al. [43]). The time, at which the sounding is reconstructed, is within three hours prior to the initiation of convective systems. For example: the reanalyzed vertical data (FNL) at 08 BST (Beijing Standard Time, BST=UTC+8 h) is revised using the surface observations at 08 and 11 BST; the vertical data at 14 BST are modified using the surface observation at 14 and 17 BST. Additionally, the revised sounding spot is within 100 km of the station or grid point that is the nearest to the convective initiation location.
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The fundamental conditions for the initiation and development of convection include moisture, instability and lifting. Additionally, the vertical wind shear is also important for the organized convection (Parker and Johnson [18]). Nine physical parameters, including dynamic, thermal and thermo-dynamic conditions, are chosen to indicate the environmental conditions three hours prior to storms: surface-based convective available potential energy (SBCAPE), most unstable convective available potential energy (MUCAPE), downdraft convective available potential energy (DCAPE), surface-based convective inhibition (SBCIN), most unstable convective inhibition (MUCIN), lifting index (LI), precipitable water from surface to 300 hPa (PWAT), 0-3 km vertical wind shear (VWS_3 km), 0-6 km vertical wind shear (VWS_6 km).
2.1. Composite radar reflectivity and severe weather reports
2.2. Classification of radar echo morphologies
2.3. Creating proximity soundings
2.4. Environmental physical parameters
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According to the definition in Section 2.2, 1640 radar echo samples from April to September of 2011-2015 are selected and classified into three main morphologies: linear systems (402 cases), cellular systems (483 cases) and nonlinear systems (755 samples). The sample numbers of the storm organizational modes are listed in Table 1. Among all the derived samples, NLs (755) are the most common, accounting for 46.03%. This percentage is similar to those (44.7%) over central east China (Zheng et al. [7]). The cellular systems combined with ICs and CCs are 483, constituting 29.45% of all the cases. All the remaining samples (402 cases, 24.51%) are linear systems. As can be seen from the pie chart in Fig. 3, the most prevalent linear systems are TSs, NSs and ELs, with percentages of 10.00%, 6.65% and 5.12%, respectively. Similar results are also found in Chen et al. [21], which focuses on the quasi-linear MCSs. The percentage of BEs is 1.34% and the smallest samples are PSs (0.79%) and LSs (0.61%). The small contribution of LSs to the total number is similar to that in central east China (Zheng et al. [7]) and the central United States (Gallus Jr et al. [27]; Duda and Gallus Jr [29]).
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In General, storm samples over south China are relatively small in April and September, while the frequency of storms is the greatest in May, with the second highest number in June (Fig. 4). The highest frequency of storms in May could be related to the pre-summer rainy season in south China (Luo [44]). For individual morphologies, the frequency of CCs is much higher than that of ICs. The two highest frequency of CC is in July and August. The two highest frequencies of TSs are in May and June, with the frequency in September being the smallest. Both LS and EL modes have their highest frequency in May, with a second peak in April. The highest frequency of BE mode is also in May, while the numbers in April and June are nearly the same. By contrast, NS mode occurs mostly in August, with June in the second place. The frequency of PS mode is relatively small throughout the study period, but there are peaks in May and August. For NL mode, the highest frequency is in May, with smaller peaks in June and August. Among the nine morphologies, the highest frequency of seven modes is in May, indicating that the convective activity in the pre-summer rainy season is the strongest.
As the frequency of each type of linear storms is small, we just discuss the duration of cellular, linear and nonlinear systems. The durations of the storms concentrate on 1-3 hours and 3-6 hours, however, the lifetimes of the different storm morphologies vary considerably (Fig. 5). The durations of linear systems are concentrated in the range of 1-3 hours, whereas those of the NL mode lie mainly between 3 and 6 hours. The case numbers of cell morphology maintaining for 1-3 hours are similar to the number of this type of convection systems that last for 3-6 hours. Compared with cellular and linear systems, there are much more events of NL mode which have lifetimes longer than 6 hours.
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To explore the environmental and circulation features of different storm morphologies, it is necessary to analyze the locations at which each category is initiated. The initiation time is defined as the time at which the maximum composite reflectivity reaches 45 dBZ and the coverage of 30 dBZ is greater than 30 km × 30 km. The initiation location is taken as the centroid point of the strongest echo or, if the strongest echoes are scattered, as the geometric center of these echoes.
In south China, IC and CC samples are mainly concentrated over coastal regions of Guangdong and Guangxi (Fig. 6). It has been found that coastal terrain and the land-sea contrast are crucial for convection initiation (Luo [44]; Wu and Luo [45]; Bai et al. [46]). The NSs occur more frequently over the coastal regions of Guangdong and the southern area of Guangxi, which is next to Beibu Gulf. Wang et al. [25] found that a mesoscale boundary between precipitation-induced cold outflows and warm air from the South China Sea and Beibu Gulf was important for the triggering of fresh convection. The TSs are generated over wider areas, with its highest frequency of occurrence being over the junction regions between Guangdong and Guangxi. The initiation locations of BEs and ELs are concentrated over the western part of Guangxi (the eastern edge of Yungui Plateau) and the coastal regions of Guangdong and Hainan, although the ELs have another high frequency in Beibu Gulf. The PSs and LSs are mainly generated in Guangdong and the coastal region (their frequency distributions are not shown in Fig. 6 because of the few samples). The NLs, which contribute the largest percentage of all the radar echoes, appear more over the coastal regions of Guangdong, the southern boundary regions of Guangdong and Guangxi, and the middle part of Guangxi. The general geographic distributions of all the categories show that storms are mainly initiated over the middle and northern regions of Guangdong (the windward slopes of the mountainous areas), the southern boundary regions of Guangdong and Guangxi, and the southern part of Guangxi (with a trumpet-shaped topography). These distributions indicate that the topography has a great influence on the convective initiation. Some case studies found that both coastal convergence and topographic lifting can influence convection initiation over the southern coast of China (Luo [44]; Chen et al. [47]; Du and Chen [48], Du et al. [49]).
Figure 6. Frequency distributions (in number of occurrences) of initiation locations for various storm morphologies: IC, CC, NS, TS, BE, EL, NL and all morphologies in sequence.
In summary, the geographical distribution of each category has the following features: the linear systems are initiated mainly over mountainous and coastal regions, the ICs tend to occur over the plains, and the CCs and NLs are more evenly distributed.
3.1. Storm organizational modes
3.2. Monthly variation and duration
3.3. Geographical distribution of convection initiation
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The combination of storm morphologies and SCW events (SDHR, severe convective winds and hail) is further investigated in this section. SDHR is an SCW type with the highest frequency and widely spread in China. Severe convective winds mostly occur in north China and Guangdong (Yang et al. [50]) whereas hails occur more frequently in mountains and plateaus, with relatively low frequency in south China (Li et al. [51]). According to the definition of SCW by the NMC, the minimum criterion for SCW is that the rainfall intensity of SDHR should be more than 20 mm h-1, but considering the local hourly precipitation intensities in south China, this is amended to 50 mm h-1 (Chen et al. [52]). When the instantaneous maximum wind reaches 17 m s-1, an SCW event is defined as severe convective wind. All the hail reports are included because of low frequency of hail in south China. The SCWs corresponding to all the radar echo samples (1640) are derived here. The main SCWs differ among the various storm morphologies (Fig. 7a). Severe convective winds "(wind"in the legend of Fig. 7) contribute the highest percentage (> 35%) of the weather phenomena induced by the ICs and CCs, and the severe convective winds percentage of IC reaches up to 50%. SDHR "(rain"in the legend of Fig. 7) and severe convective winds are the most common weather phenomenon associated with the TSs and BEs: the percentage of rain being higher than 45% and severe convective winds accounting for more than 25%. The main samples of LSs and Els produce SDHR (with respective percentages being ~70% and 45%), while the severe convective wind percentages are about 10%. Similar to the SCW associated with the PS mode described in Zheng et al. [7], there are no hail events associated with the PS mode in central east China, which contrasts with the significant hail reports in the United States. It is also clearly shown that hail events only appear in IC, CC and NS systems, but NS and BE systems are the leading producers of hail events in central east China (Zheng et al. [7]). SDHRs and severe convective winds are associated with just a small percentage of this type of radar echo. SDHR accompanying with severe convective winds could occur in all the morphologies (Fig. 7b). ICs and CCs can produce SDHR and hail events simultaneously. For CCs, TSs and NSs, hail could appear with SDHR and severe convective winds at the same time.
Figure 7. Percentages of different weather phenomena associated with various storm morphologies (the precipitation criterion is a minimum of 50 mm h-1). (a) Percentages of each weather phenomenon; (b) percentages of various weather phenomena occurring simultaneously.
On the other hand, Fig. 8 illustrates the percentage distributions of storm morphologies for the three main SCW events. For severe convective winds, the CC mode accounts for the highest percentage, with the NL mode in the second place (Fig. 8a). This feature is partly similar to the results in north China, while the percentage of CCs is the highest associated with severe convective winds. In central east China, however, BE systems had the highest probability of severe convective winds, especially significant severe convective winds (≥ 24 m s-1) (Zheng et al. [7]). It was also demonstrated that bow echoes tended to produce more severe convective winds reports in the United States (Gallus Jr et al. [27]). However, since the number of samples of the NLs is much greater than those of other morphologies, the percentage of severe convective winds cases is not high among NL mode samples. The percentages for the ICs and TSs are near 10%. SDHR is mostly associated with the NLs, while the CCs, and TSs each account for more than 10% (Fig. 8b). The proportions of other storm morphologies are below 10%. The highest percentage of hail is associated with the CCs (> 40%), while the ICs, NSs and NLs each account for more than 10% (Fig. 8c).
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The physical parameters listed in section 2.4 are related to moisture conditions (PWAT), thermal (SBCAPE, MUCAPE, DCAPE, SBCIN, MUCIN, LI, etc.), and dynamic (VWS_3km, VWS_6km) conditions.
Table 2 lists the average physical parameters of all linear systems. A comparison among these parameters shows that the BE mode has the highest values of SBCIN and MUCIN (thermal conditions) and of VWS_ 6km (dynamical conditions), indicating that when more unstable energy is accumulated before the initiation of convection, accompanied by simultaneous intense vertical wind shear, the convection can develop into strong convective systems after initiation. The TSs account for the highest percentage of general linear modes. From a comparison of its parameters with those of other morphologies, it is found that the absolute LI of the TS mode is the second greatest, but the vertical wind shear (VWS_3km and VWS_6km) is not very intense. For this mode, SBCAPE, DCAPE and the moisture conditions (PWAT) all lie in the middle range. After the TS mode, the NS mode has the greatest number of linear samples. This mode is associated with a high frequency of occurrence of severe convective winds and hail, characterized by strong updraft and downdraft (as indicated by the large SBCAPE and DCAPE and small SBCIN) and weak vertical wind shear (as indicated by the small VWS_3km and VWS_6km). These environmental conditions indicate that the NSs occur in environments with high convective energy and weak vertical wind shear, causing weak tilting of vertical motion, which can explain the non-stratiform region. Among the other morphologies, the ELs have the smallest SBCAPE and the second smallest DCAPE, but relatively large SBCIN and MUCIN, which means that this convection system needs strong triggering conditions for its development. The high PWAT of the ELs means that this system occurs when moisture conditions are favorable. The environmental wind vertical shear of the ELs has a medium value, which is greater than those of the TS and NS modes but smaller than that of BE mode.
Type SBCAPE (J kg-1) MUCAPE (J kg-1) DCAPE (J kg-1) MUCIN (J kg-1) SBCIN (J kg-1) LI (K) VWS_3km (m s-1) VWS_6km (m s-1) PWAT (mm) BE 1382.1 1251.5 618.7 69.8 75.4 -3.0 17.1 26.5 4.3 TS 1843.0 1785.9 570.0 49.7 54.1 -3.5 14.4 21.2 4.1 NS 2093.0 1982.4 663.7 41.9 49.6 -3.5 13.3 20.6 3.8 EL 1276.3 1168.3 549.4 61.9 69.3 -2.3 16.8 24.8 4.3 LS 2114.4 2092.6 678.4 41.1 51.9 -3.8 17.2 24.7 3.7 PS 1362.5 1351.6 364.6 18.0 31.3 -2.3 18.3 26.1 4.6 Table 2. Average physical parameters of various linear morphologies.
Owing to the limited number of samples of the LSs in south China, it is possible that the features of the parameters may be affected to a certain extent. According to the results of the present calculation, the large SBCAPE, DCAPE and MUCAPE imply strong unstable energy, similarly to the NSs. Additionally, the small PWAT (3.7cm) reveals that the LSs mostly occur in relatively dry environments. The environmental wind shear (VWS_3km) of LSs are larger than that of other morphologies, which means that for the LSs to occur, high energy and strong vertical wind shear are necessary. This may be the reason of the low frequency of occurrence of LSs. The frequency of the PSs is even lower than that over central east China (Zheng et al. [7]). Compared with the environmental conditions of the LSs, the PSs have much lower SBCAPE, DCAPE and SBCIN but higher PWAT. Moreover, the vertical wind shear parameters are larger than those of other morphologies. These characteristics indicate that the derived PSs are mostly generated in wet environments featuring low convective energy but strong vertical wind shear.
In addition to the different SCW events associated with linear systems, cellular systems and nonlinear systems, respectively, there are also differences among their environmental parameters (Table 3). First of all, SBCAPE, MUCAPE, LI and other thermal and dynamic parameters of cellular systems are much larger than those of linear and nonlinear systems, suggesting that high values of thermal and unstable energy are more favorable for the initiation of cellular systems. Furthermore, the larger DCAPE of cellular systems indicates that stronger downdraft could produce severe convective winds and hail. Meanwhile, the smaller PWAT of cellular systems suggest that these occur in relatively dry environment with lower amounts of water vapor. Vertical wind shear (VWS_3km and VWS_6km) of the cellular systems is weaker than linear and nonlinear systems. It is possible that cellular systems (CCs and ICs) are more favorable to be initiated under favorable thermal environmental conditions. The small SBCAPE of linear systems indicates that relatively low energy could also trigger this type of convection. The higher DCAPE of linear systems compared with nonlinear systems indicates a greater likelihood of severe convective winds for the former. On the other hand, the stronger vertical wind shears of linear systems imply a well organization of convection systems (Parker and Johnson [18]). The greater enrollment of mid-level dry air induces a high energy of downdraft (DCAPE). These environmental parameters of nonlinear systems are in the middle range compared with the other two morphologies.
Type SBCAPE (J kg-1) MUCAPE (J kg-1) DCAPE (J kg-1) MUCIN (J kg-1) SBCIN (J kg-1) LI (K) VWS_3km (m s-1) VWS_6km (m s-1) PWAT (mm) Linear 1768.0 1684.5 590.8 49.7 56.2 -3.2 14.9 22.3 4.1 Cellular 2558.4 2522.4 688.6 25.4 32.7 -4.4 11.5 18.2 3.4 Nonlinear 1974.9 1867.8 554.3 40.5 47.4 -3.6 13.6 20.9 4.1 Table 3. Comparison of environmental parameters of three storm morphologies.
The above results demonstrate that each morphology not only produces different SCW events, but also corresponds to different environmental conditions before convection is initiated. Overall, cellular systems tend to occur in the environment with favorable thermal condition, substantial unstable energy and low PWAT, whereas the environmental conditions favoring the initiation of linear systems feature strong vertical wind shear, high PWAT, and intense SBCIN. The environmental parameters favoring the initiation of nonlinear systems are between those of the other two morphologies. In addition, large DCAPE values of cellular and linear systems indicate a high probability of severe convective winds produced by downdraft. Therefore, further exploration of morphologies is important for understanding the three-dimensional structure, their associated SCWs and the mechanisms involved in the initiation and maintenance of convection systems.
Table 4 presents a comparison of environmental conditions before convection initiation over different areas. The morphologies of linear systems over central east China and the United States are the same as those in previous studies (Zheng et al. [7]; Bluestein and Jain [22]). The SBCAPE (1768 J kg-1) of linear systems over south China is smaller than that over central east China in Zheng et al. [7], but is larger than the SBCAPE of squall lines (1568 J kg-1) over east China in Meng et al. [19] and that of the convective systems over central United States (Parker [28]). Additionally, the SBCIN (56.2 J kg-1) is clearly higher than that over central east China (34 J kg-1, Zheng et al. [7]) and Oklahoma (33 J kg-1, Parker [28]), implying that the initiation of convection needs substantial accumulated unstable energy. LI over south China is similar to that of the squall lines over east China in Meng et al. [19], but it is lower than that over central east China in Zheng et al. [7] with more unstable environmental conditions. Among the moisture conditions, the PWAT of linear systems over south China is smaller than that over central east China and east China but is larger than that over Oklahoma and central United States.
Regions Environmental parameters SBCAPE (J kg-1) SBCIN (J kg-1) LI (K) PWAT (cm) South China This study Lines 1768 56.2 -3.2 4.1 Cells 2558 32.7 -4.4 3.4 No-Lines 1974 47.4 -3.6 4.1 YHRV Zheng et al. [7] All events 2188 23 -5.0 5.2 Lines 1820 34 -4.3 5.4 East China Meng et al. [19] Squall lines 1568 61 -4.0 5.9 Oklahoma Bluestein and Jain [22] Lines 2260 33 - 2.8 Central plains of Unites States Parker and Johnson [18] LS 1009 - -3.5 3.3 PS 813 - -2.2 2.4 TS 1605 - -5.4 3.4 Table 4. Comparison of system environmental parameters from different studies.
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Composite radar reflectivity data during April to September from 2011 to 2015 have been used to investigate and classify storms and their environmental conditions in south China (18-27° N, 105-120° E). The derived storms have been divided into three main types, including linear, cellular and nonlinear systems. According to the relative locations of linear convection and stratiform region, the linear systems have been subdivided into six morphologies, including TS, BE, LS, EL, NS and PS. And then, the SCW events corresponding to each morphology have been categorized. Finally, the thermal, dynamic and water vapor environmental parameters of the three main types have been compared.
The proportion of NLs of all the total radar echoes is 46.03%. Cellular systems account for 29.45%, which is higher than that of linear systems (24.51%). Among the linear systems, the frequencies of TSs and NSs are high, whereas there are only small samples of the LSs and PSs. The monthly variation of storms show that a high frequency of convection appears in May, followed by June. The sample numbers in April and September are both small. From the geographic distribution, it is found that the maximum frequency occurs over the central and northern regions of Guangdong (the windward slopes of mountainous areas), coastal regions, the boundary regions between Guangdong and Guangxi, and the southern regions of Guangxi (with a trumpet-shaped topography), indicating the significant effect of topography on convective systems.
The main SCW events differ among the various storm morphologies. Severe convective winds account for the highest percentage (35%) of the SCW events induced by the ICs and CCs. SDHR and severe convective winds are the most common weather events associated with the TSs and BEs: the percentage of rain being higher than 45% and that of severe convective winds more than 25%. For the NSs, hail can occur simultaneously with SDHR and severe convective winds. SDHR is the most common weather event associated with the NLs, and the percentage of severe convective winds is relatively small. Comparisons of environmental physical parameters show that cellular convection systems tend to occur in the environment with favorable thermal condition, substantial unstable energy and low PWAT water vapor. However, the environmental conditions favoring the initiation of linear systems feature strong vertical wind shear, high PWAT, and intense SBCIN. The environmental parameters favoring the initiation of nonlinear systems are between those of the other two types of morphologies.
Based on the different features of morphologies, their associated SCW events and environmental conditions of storms over south China and their three-dimensional structural characteristics and evolutionary pathways will be analyzed and explored in the future study. Additionally, the synoptic patterns in low - and mid-troposphere and surface mesoscale system related to the storms are also to be analyzed to understand their formation and development mechanism.