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The Guangzhou radar became operational in May 2016. The radar operates in the conventional VCP21 volume-scan mode and completes a volume scan using nine specific elevation angles (0.5°, 1.5°, 2.4°, 3.3°, 4.3°, 6.0°, 9.9°, 14.6°, and 19.5°) in 6 min. The parameters of the radar are presented in Table 1.
Variable Parameter Antenna diameter 8.5 m Antenna gain ≥44 dB Bean width 0.95° Frequency 2885 MHz Peak power ≥325 kW Pulse width 1.57 us, 4.7 us Pulse repetition frequency 322 Hz-1304 Hz Work model Simultaneously transmit and receive Minimum detectable power ≤−109 dBm (1.57 us) ≤−114 dBm (4.7 us) Noise ≤4 dB Dynamic range ≥85 dB Range resolution 250 m/1000 m Observation accuracy Z≤ 1dB ZDR ≤ 0.2dB ΦDP ≤ 2° KDP ≤ 0.2° km-1 ρHV (0) ≤ 0.001 Table 1. The main technical parameters of the Guangzhou dualpolarization radar.
From March 1 to October 30, 2017, the Guangzhou Radar observed 67 rainfall events with the rain gauges in the 100 - range of the Guangzhou radar observed precipitation, such as squall lines and typhoons. The maximum rainfall rate was 183.4 mm h-1. In total, there are 48, 271 records of hourly rainfall rates that were greater than 1-mm h-1, 22, 189 records of 1-5-mm h-1, 13, 171 records of 5-10 - mm h-1, 8, 839 records of 10-20 - mm h-1, 3, 854 records of 20-50-mm h-1, and 274 records of more than 50 - mm h-1. Table 2 (see the appendix) presents the duration and types of rainfall events with a duration more than 5 hours.
No. Date and Time (China Standard Time) Duration (h) Precipitation Type 1 07:00 March 7 to 12:00 March 8 29 Stratus 2 05:00 March 9 to 20:00 March 10 39 Stratus 3 04:00 March 11 to 11:00 March 12 31 Stratus 4 01:00 March 18 to 23:00 March 19 46 Stratocumulus 5 00:00 to 21:00 March 22 21 Stratus 6 21:00 March 28 to 13:00 March 29 14 Stratocumulus 7 00:00 March 31 to 01:00 April 1 25 Stratocumulus 8 08:00 to 23:00 April 11 15 Stratocumulus 9 16:00 to 23:00 April 12 7 Stratocumulus 10 10:00 April 19 to 02:00 April 20 16 Stratocumulus 11 10:00 April 20 to 20:00 April 21 34 Stratocumulus 12 08:00 April 22 to 23:00 April 23 39 Stratus 13 20:00 April 24 to 07:00 April 27 59 Stratocumulus 14 18:00 to 23:00 May 2 5 Convective Clouds 15 04:00 to 11:00 May 4 7 Stratocumulus 16 00:00 to 20:00 May 7 20 Stratocumulus 17 16:00 to 23:00 May 8 7 Stratocumulus 18 07:00 to 12:00 May 12 5 Convective Clouds 19 17:00 May 14 to 06:00 May 16 37 Stratocumulus 20 15:00 to 21:00 May 21 6 Stratocumulus 21 18:00 to 23:00 May 23 5 Convective Clouds 22 06:00 to 13:00 May 24 7 Stratocumulus 23 09:00 to 15:00 June 9 6 Stratocumulus 24 02:00 to 13:00 June 14 11 Stratocumulus 25 18:00 June 15 to 13:00 June 18 65 Stratocumulus 26 12:00 to 17:00 June 19 5 Convective Clouds 27 10:00 to 22:00 June 20 12 Stratocumulus 28 13:00 to 22:00 June 21 9 Stratocumulus 29 12:00 to 19:00 June 23 7 Stratocumulus 30 00:00 July 2 to 16:00 July 4 64 Stratocumulus 31 12:00 to 18:00 July 5 6 Convective Clouds 32 10:00 to 18:00 July 6 8 Convective Clouds 33 12:00 to 20:00 July 8 8 Convective Clouds 34 12:00 to 17:00 July 10 5 Convective Clouds 35 08:00 to 18:00 July 11 10 Convective Clouds 36 13:00 to 21:00 July 13 8 Convective Clouds 37 14:00 July 15 to 03:00 July 19 85 Stratocumulus 38 10:00 to 20:00 July 19 10 Stratocumulus 39 13:00 to 20:00 July 21 7 Convective Clouds 40 00:00 July 23 to 01:00 July 24 25 Stratocumulus 41 17:00 August 1 to 17:00 August 2 24 Convective Clouds 42 09:00 to 19:00 August 3 10 Convective Clouds 43 10:00 to 15:00 August 11 5 Convective Clouds 44 13:00 August 22 to 22:00 August 24 57 Stratocumulus 45 17:00 August 26 to 19:00 August 28 50 Stratocumulus 46 05:00 to 23:00 September 4 18 Stratocumulus 47 11:00 September 5 to 00:00 September 6 13 Convective Clouds 48 08:00 to 17:00 September 7 9 Convective Clouds 49 14:00 to 19:00 September 21 5 Convective Clouds 50 13:00 to 18:00 September 29 5 Convective Clouds 51 17:00 October 15 to 20:00 October 16 27 Stratocumulus Table 2. Rainfall events from March 1 to October 30, 2017.
In this study, the DSD data from 8 OTT disdrometers and 3 Metstar (Beijing Metstar Radar Co., Ltd.) disdrometers in Guangdong in 2014, 2016, and 2017 were used to fit the QPE estimators. After the quality control procedure (Zhang et al. [16]), there were 17, 326 1-min valid DSD samples. The spatial distribution of the disdrometers is depicted in Fig. 1. The hourly rainfall data measured by more than 1600 rain gauges in Guangdong Province were used to evaluate QPE.
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After Guangzhou radar construction, a series of tests, such as built-in testing, sun-calibration, and vertical pointed calibration were conducted by the Meteorological Observation Center, China Meteorological Administration. And the result of the test indicated that ZDR accuracy is better than 0.2 dB (Chen et al. [17]). The quality control of the radar data was conducted prior to performing the radar QPE as follows:
(1) noise correction for ρHV (0) and ZDR based on the assumption that the horizontal and vertical channel noise levels of the dual-polarization radar are consistent (Liu et al. [18]);
(2) all data with ρHV (0) < 0.7, Z > 40 dB and absolute value of radial velocity less 0.5 m s-1 were removed to exclude non meteorological echoes;
(3) all negative values of ZH, ZDR and KDP were removed, and the values of ZH, and ZDR were smoothed over 5 range gates to remove noisiness in the raw data, particularly for ZDR;
(4) in this study, KDP is estimated by ΦDP using the algorithm like the one in Wang et al. [19] after 5-gate smoothing filter was applied to the basic ΦDP data in each ray.
The CAPPI reflectivity at a 3 - km altitude with a horizontal resolution of 0.01° × 0.01° is used in DRVCQPE, while the remaining radar QPE algorithms use hybrid scanning. When the scanning data at elevation 0.5° is blocked, data with higher layer will be used, and so on.
Additionally, the processing of DSD data in this study refers to the method reported by Zhang et al. [20]. The assessment requires consecutive observation records by the rain gauge for 24 hours; otherwise, the automatic station would be considered to be unreliable and would be rejected.
2.1. Data resource
2.2. Data preprocessing and quality control
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The QPE that uses dual-polarization radar data mainly includes four basic estimator, including R(ZH), R (ZH, ZDR), R(KDP), and R(KDP, ZDR). The estimators are as follows:
$$ {R({Z_H}) = {a_1} \times {Z_H}^{{b_1}}, } $$ (1) $$ {R({K_{{\rm{DP}}}}) = {a_2} \times K_{{\rm{DP}}}^{{b_2}}, } $$ (2) $$ {R({Z_H}, {Z_{{\rm{DR}}}}) = {a_3} \times Z_H^{{b_3}} \times {{10}^{{c_3} \times {Z_{{\rm{DR}}}}}}, }\ $$ (3) $$ {R({K_{{\rm{DP}}}}, {Z_{{\rm{DR}}}}) = {a_4} \times K_{{\rm{DP}}}^{{b_4}} \times {{10}^{{c_4} \times {Z_{{\rm{DR}}}}}}, } $$ (4) where a, b, and c are the coefficients; R is the rainfall rate in mm h-1; ZH is the reflectivity factor in mm6 m-3.
In the case of light rain, the polarization parameters of Z DR and KDP are observed to be relatively small with a few obvious fluctuations that can be attributed to noise (Chen et al. [17]); therefore, R (ZH, ZDR), R (KDP), and R (KDP, ZDR) exhibit no advantages over the R (ZH) method in this case (Chandrasekar et al. [1]). As the rainfall rate increases, the deformation of raindrops becomes significantly reduced. ZDR is the polarization parameter that characterizes this deformation information. Hence, the R (ZH, ZDR) and R (KDP, ZDR) based on Z DR exhibit significant advantages, and Ryzhkov et al. [5] depicted that R (KDP, ZDR) resulted in considerably accurate predictions with respect to precipitation in case of medium to high intensities. With a further increase in rainfall intensity, especially when the precipitation contains non-liquid forms, R (KDP) provides distinctively accurate estimations because the parameter that characterizes the phase variability of the radar beam after it passes through the precipitation particles, KDP, is considerably resilient to the attenuation and particle phase effects (Chandrasekar et al. [1]).
Currently, the dual-polarization radar QPE is usually performed by combining these estimators, which can be referred to as the optimization algorithm. The localized JPOLE algorithm (Ryzhkov et al. [3]), the localized CSU-HIDRO (Cifelli et al. [4]), and the HCAQPE algorithm proposed in this study are all optimization algorithms.
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To develop an optimization algorithm, it is first necessary to localize the estimators. Based on the DSD data observed in Guangdong, the estimator coefficients that are suitable for the annually first rainy season and annually second rainy season (July to September) in Guangdong were fitted by using the piecewise fitting method (Zhang et al. [16]). The results are listed in Tables 3 and 4. In this study, the HCA suggested by Wu et al. [12] was used to classify the hydrometeors, and we divided the classification results into liquid, mixedphases, and ice, and we subsequently combined the polarimetric parameters to guide the choice of estimators. The HCA-QPE algorithm flowchart is depicted in Fig. 2, where NaN represents an invalid value. An analysis of the polarization radar data indicates that noise can easily affect the ZDR and KDP when the SNR is < 20 dB, leading to large spatiotemporal variations (Chen et al. [17]). Therefore, the R1 (ZH) used for light rain (Zhang et al. [20]) is used to perform the estimation under these SNR conditions because the Z DR and KDP are not appropriate for light rain estimation. In this study, the threshold of ZH is the same with CSU-HIDRO algorithm (Cifelli et al. [4]), and after a large number of experiments, the threshold of ZDR and K DP are concluded (Fig. 2).
Estimators Coefficient a Coefficient b Coefficient c R1(ZH) 0.0082 0.749 R2(ZH) 0.0154 0.7681 R1(KDP) 30.30 0.9298 R2(KDP) 33.6142 0.8332 R(ZH, ZDR) 0.0084 0.9284 −0.4055 R(KDP, ZDR) 51.16 0.9311 −0.0852 Table 3. The QPE estimator coefficients of the annually first rainly season.
Estimators Coefficient a Coefficient b Coefficient c R1(ZH) 0.03966 0.6246 R2(ZH) 0.0135 0.7923 R1(KDP) 33.82 0.8678 R2(KDP) 46.29 0.8941 R(ZH, ZDR) 0.00892 0.9078 −0.3573 R(KDP, ZDR) 60.5 0.9638 −0.124 Table 4. The QPE estimator coefficients of the annually second rainy season.
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The CSU-HIDRO algorithm has been described in Cifelli et al. [4]. In this paper, we used the HCA suggested by Wu et al. [12] as the guide of the choice of the estimators. And the coefficients of each estimator were refitted using the DSD data recorded in Guangdong. The results are listed in Tables 5 and 6.
Estimators Coefficient a Coefficient b Coefficient c R(ZH) 0.0082 0.749 R(KDP) 32.2886 0.8991 R(ZH, ZDR) 0.0047 0.9624 −0.3574 R(KDP, ZDR) 52.656 0.9721 −0.0996 Table 5. The QPE estimator coefficients of the annually first rainy season.
Estimators Coefficient a Coefficient b Coefficient c R(ZH) 0.03966 0.6246 R(KDP) 35.69 0.8376 R(ZH, ZDR) 0.01014 0.9029 −0.3739 R(KDP, ZDR) 60.8 0.9516 −0.1241 Table 6. The QPE estimator coefficients of the annually second rainy season.
According to the JPOLE (Ryzhkov et al. [3]) optimization algorithm, the choice between various estimators is determined solely by the rainfall rate computed from R (ZH) relation. In this paper, the coefficients of each estimators were refitted using the DSD data recorded in Guangdong. The results are listed in Tables 5 and 6. Because the JPOLE algorithm uses rainfall rate as a threshold to select different QPE estimators, R(KDP), R(ZH, ZDR), and R(KDP, ZDR) may provide invalid or large false values when ZDR or KDP is either small and unstable or negative. To avoid this, R (ZH) is used as the final QPE result under the aforementioned conditions.
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Because of the variation in the DSD of precipitation and the error of reflectivity factor, it is impossible to obtain a stable Z-R relation. Currently, the dynamic Z-R relations algorithm is used for the radar QPE in China (Wang et al. [13]; Chen et al. [21]). To further improve the accuracy of radar QPE, the variational correction method (Zhang et al. [22]) is applied to the operational dynamic Z-R relations algorithm in Guangdong Province.
In this paper, a total of 810 rain gauges that were randomly chosen from half of the gauges in the coverage of the Guangzhou radar volume scan were used. Because this is a QPE algorithm for operational services in Guangdong Province, the parameters a and b of Z = a × Rb were time-averaged value before the period considered in this study, i. e., before 00: 00 March 1, 2017. The starting values were 16 and 2.45. Furthermore, the Z-R coefficients were refitted every 60 minutes and were used for the subsequent 6-min radar QPE. From March 1 to October 30, 2017, the value of a fluctuated between 16 and 250, and the value of b fluctuated between 1.2 and 2.85.
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The radar QPE results were evaluated using the mean absolute error (AE), the average relative error (RE), the ratio deviation (BIAS) and the root mean square error (RMSE). These parameters are calculated as:
$$ {{\rm{AE}} = \frac{1}{n}\sum\limits_{i = 1}^n | {G_i} - {R_i}|, } $$ (5) $$ {{\rm{RE}} = \frac{{\frac{1}{n}\sum\nolimits_{i = 1}^n {{G_i} - {R_i}} }}{{\frac{1}{n}\sum\nolimits_{i = 1}^n {{G_i}} }}, } $$ (6) $$ {{\rm{BIAS}} = \frac{{\frac{1}{n}\sum\nolimits_{i = 1}^n {{R_i}} }}{{\frac{1}{n}\sum\nolimits_{i = 1}^n {{G_i}} }}, } $$ (7) $$ {{\rm{RMSE}} = \sqrt {\frac{1}{n}\sum\limits_{i = 1}^n {{{({G_i} - {R_i})}^2}} } , } $$ (8) where G i denotes the 1-h observed rainfall of the i-th rain gauge sample in the evaluation data set, Ri denotes the 1-h estimated rainfall with radar, and n denotes the number of effective QPE-rain gauge pairs.
Because the DRVC-QPE algorithm requires rain gauges to correct retrieved rainfall rate, all of rain gauges are divided nto two group; one is for correction and the other is for evaluation. Because of the R (ZH), HCA-QPE, CSU-HIDRO, and JPOLE algorithms in this study did not use the rain gauges rainfall for real-time correction, the evaluation station can simply be selected from within a given distance range.
3.1. HCA-QPE algorithm
3.2. Localized CSU-HIDRO and JPOLE algorithms
3.3. Operational QPE algorithm in Guangdong Province (dynamic Z-R relations based on variational correction QPE algorithm (DRVC-QPE))
3.4. Evaluation methods
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The QPEs with HCA-QPE, CSU-HIDRO, JPOLE, and DRVD-QPE algorithms were performed for rainfall events from March 1 to October 30, 2017 shown in Table 2. The dual-polarization radar QPE capability is evaluated in different rainfall levels and range from radar site.
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In this analysis, the hourly rainfall measured by the rain gauges can be divided into 5 levels, including 1- 5mm, 5-10mm, 10-20mm, 20-50mm, and 50mm and above. Table 7 presents the results using the HCA-QPE, CSU-HIDRO, JPOLE, DRVC-QPE, and R (ZH) algorithms for five rain fall levels.
Precipitation Estima‐ tion Algorithm Evaluation Method Hourly Rainfall (mm) Average 1-5 5-10 10-20 20-50 ≥50 HCA-QPE RE (%) 65.43 38.07 32.07 26.93 24.64 47.99 AE (mm) 1.58 2.69 4.45 7.53 15.87 3.19 RMSE (mm) 2.82 3.52 5.66 9.39 19.0 5.19 BIAS 1.35 0.96 0.88 0.83 0.74 0.93 HCA-QPE RE (%) 53.78 45.75 39.44 35.32 36.94 49.92 AE (mm) 1.47 3.26 5.48 10.12 33.35 3.94 RMSE (mm) 2.45 4.12 6.54 11.87 26.3 6.28 BIAS 0.87 0.73 0.7 0.69 0.64 0.71 HCA-QPE RE (%) 52.89 41.82 38.88 35.73 34.29 48.85 AE (mm) 1.4 2.91 6.53 10.26 24.32 3.83 RMSE (mm) 2.39 3.73 7.3 12.2 31.74 6.18 BIAS 1.02 0.78 0.71 0.69 0.67 0.75 HCA-QPE RE (%) 56.45 46.28 40.96 41.17 48.56 50.15 AE (mm) 1.31 3.3 5.76 11.93 30.34 3.31 RMSE (mm) 2.71 4.28 7.2 14.32 34.2 6.22 BIAS 1.12 0.84 0.71 0.64 0.54 0.78 R (ZH) RE (%) 47.12 54.73 53.85 52.8 57.5 50.96 AE (mm) 1.4 3.91 7.53 15.28 36.36 5.03 RMSE (mm) 1.93 4.32 8.19 16.62 37.94 8.01 BIAS 0.77 0.69 0.6 0.53 0.49 0.56 Table 7. The QPE evaluation results from March 1 to October 30, 2017.
Previous studies have demonstrated that the fixed Z-R relationship R (ZH) underestimated all types of precipitation (Gou et al. [23]). Although the R(ZH) is fitted from local DSDs data in Guangdong, the QPE is also underestimated. It can be observed from Table 7 that the maximum BIAS for R (ZH) is 0.87. The BIAS gradually declined with the rainfall rate. For a rainfall rate >50mm h-1, the BIAS is only 0.49. The DRVC-QPE algorithm considerably improved the underestimation due to the corrections by rain gauge data. The BIAS increased by 28.2% in total while the root-mean-square error (RMSE) was reduced by 22.4% (1.79 mm). However, for the 1-5mm h-1 rainfall rate, the DRVCQPE is overestimated (BIAS is 1.12) with large values of RE and RMSE.
Despite the fact that the HCA-QPE algorithm proposed in this study did not use the rain gauges data to correct the QPE results, the RE decreased by 4.3% on average, the AE reduced by 3.6% (0.12 mm) on average, and the RMSE declined 16.6% (1.03 mm) on average, whereas BIAS increased by 16.1% on average as compared with those obtained using the DRVC-QPE algorithm. However, the HCA-QPE algorithm shows a larger error as compared with that showed by the DRVCQPE algorithm when the rainfall rate was less than 5mm h-1, which was mainly due to overestimation (BIAS being 1.35). When the rainfall rate is more than 5mm h-1, the error of the HCA-QPE algorithm is evidently better than that of the DRVC-QPE algorithm. As the precipitation intensified, the accuracy improved even more. At a strong rainfall rate (over 20mm h-1), HCAQPE has its RE, AE, and RMSE reduced by 34.5%, 36.9% (4.4 mm), 34.3% (4.93 mm), and BIAS increased by 29.7% as compared to that of the DRVC-QPE algorithm.
The localized CSU-HIDRO and JPOLE algorithms, in the absence of the corrections by measured rainfall data, still performed better than the DRVC-QPE algorithm when rainfall rate is more than 5mm h-1; however, the rainfall rate of the localized CSU-HIDRO and JPOLE algorithms are still underestimated. The HCA-QPE algorithm proposed in this study showed the least error as compared with that by other algorithms for rainfall rates more than 5mm h-1; furthermore, the higher the rainfall rate, the better the performance. Additionally, the HCA-QPE algorithm considerably improved the underestimation that was observed in other algorithms.
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The U.S. National Weather Service (NWS) requires its S-band dual-polarization radar QPE to cover a region of 230km around the radar (Ryzhkov et al.[24]). Although we did not explicitly regulate the coverage distance, the CINRAD-SA radar products generally cover 230km for the networking between multiple radar products.
Because the CINRAD-SA dual polarization radars show a minimum scan elevation angle of 0.5°, the vertical height increases as the horizontal distance from the radar increases. Due to the increase in precipitation or evaporation, the movement of airflow, the phase change of particles, and so on, the radar observation will be altered in the vertical direction. This shift will increase with horizontal distance from the radar and with vertical distance from the ground (Shi et al. [25]).
In the melting layer, the reflectivity factor, may be 5-10dB higher inside the bright-band due to melting, collision, and slow falling speed of the snowflakes (Dai et al. [26]). Majority of the hydrometeor above the melting layer would be dry snowflakes and ice crystals with weak backscattering, which causes a decrease in the reflectivity factor and the differential reflectivity. Especially in the heights above the melting layer, the radar SNR is observed to be generally small. All the aforementioned reasons will cause the QPE results to alter with distance.
To analyze the variation characteristics of error with distance in the HCA-QPE, CSU-HIDRO, and JPOLE algorithms, this study categorized the automatic stations in the radar coverage into 9 groups at a 25-km interval with the furthest being 225km. Radar QPE was conducted for various types of precipitation from March 1 to October 30, 2017 at each distance range. BIAS and RMSE were further calculated over each distance range. Fig. 3 depicts the variation of BIAS and RMSE along the distance ranges of the three optimization algorithms.
The observed facts from the sounding data of 2017 (59280) indicate that the height of the 0 ℃-layer during the rainy seasons in Guangdong is 3-5.5km. Based on the assumption of the standard atmosphere, the calculated horizontal distance range corresponding to the 0 ℃-layer at an elevation angle of 0.5° should be approximately 160-236km. By considering its thickness (Gatlin et al. [27]; Emory et al. [28]), the melting layer may have an impact at a horizontal distance of ≥125km.
As depicted in Fig. 3, the radar QPE estimation results of the three optimization algorithms are smaller than the actual results (BIAS less than 1) in the range of 0-225km. The HCA-QPE algorithm is better than the other two optimization algorithms (minimum RMSE) across all the distance ranges. The three optimization algorithms perform an even better estimation in the range of 50-125km than in other ranges. That is because the influence of the grounding and melting layers on the echo is small and the QPE results are mainly affected by the distribution of raindrops and hail.
As the horizontal distance extends to approximately 125km, the radar QPE results begin to be affected by the melting layer. Based on the results of this study, the three radar QPE optimization algorithms did not show a consistent increase in and above the melting layer. There is a certain fluctuation from 125km to 200km. Beyond 200km, the altitude is close to the top of the melting layer and the majority of the hydrometeors above the melting layer comprises dry snowflakes and ice crystals with a weak backscattering effect. This would induce a decrease in the reflectivity and the differential reflectivity. Because the specific differential propagation phase reduces while passing through the non-liquid region, the estimation results tend to be small. In any case, it can clearly be observed from Fig. 3b that the RMSE of the three optimization algorithms increases rapidly while reaching the melting layer or beyond, indicating that the existence of the melting layer reduces the accuracy of QPE.