A significant part of Hong Kong has hilly terrain with relatively short flow concentration time and, hence, is susceptible to the threat of flash floods and landslides during intense convective thunderstorms and tropical cyclones. For places like Hong Kong, a rainfall model that could adequately capture small-scale temporal and spatial variations would be highly desirable. The main challenge in rain-field modeling is to capture and describe the dynamic time-space evolution of the rainfall during rainstorm events. In this study, radar data with a high spatial (1 km^{2}) and temporal (6 min) resolution of four rainstorm events in Hong Kong are analyzed. A geostatistical approach based on indicator variograms of rain-fields is used. The spatial structure of a rain-field is found to be highly anisotropic and should be adequately considered in the model. Variability of the spatial structure of a rain-field was described well by the main features of the variograms. Moreover, it is possible to identify whether multiple rainstorm centers exist by comparing the mean length and range. In order to establish reliable statistics on the spatial and temporal structure of rain-fields in Hong Kong, this approach could be applied to a large set of rainstorm events in this same region in the future.

## INTRODUCTION

Hong Kong is small in size but complex in topography. There are extensive mountain ranges with substantial altitude variations scattered throughout the Territory. These areas and catchments have a relatively short flow concentration time and are particularly susceptible to the threat of flash floods and landslides during intense convective thunderstorms and tropical cyclones. For places like Hong Kong, a rainfall model that could adequately capture small-scale temporal and spatial variations of rain-fields would be highly desirable. In rain-field modeling, the main challenge is to capture and describe the dynamic time-space evolution of the rainfall during rainstorm events.

However, most current models make simplified assumptions about the way rainfall fields evolve, like space homogeneity and weak time dependency. A false assumption of a stationary model may lead to unreliable estimation. This kind of model cannot be expected to preserve important statistical features of the actual rainstorm events, in particular, at finer temporal and spatial scales. Furthermore, the orographic effect on the rainfall amount has been clearly observed across the Hong Kong Territory. A rainfall model that can consider non-stationarity in space would be desirable and useful.

It has long been acknowledged that the intensity of precipitation is highly variable over space and time in mountain environments (Castro *et al.* 2014). An understanding of the space-time structure of rain-fields is of great importance for storm modeling, runoff prediction, and subsequent hydraulic structural design (Abedini *et al.* 2013; Kang & Merwade 2014; Shafiei *et al.* 2014; Xu *et al.* 2015). Arnaud *et al.* (2002) estimated the peak flows and runoff volumes from the distributed hydrological models using different patterns of rainfall as input (namely, spatially averaged uniform rainfall and non-uniform rainfall) and studied the influence of the spatial variability of rainfall on the estimation of runoff characteristics. They concluded that runoff volumes and peak flows could be affected considerably by the spatial variation of rainfall patterns, as well as the runoff production model, the size of the catchment, and the frequency of the event. Le Lay & Saulnier (2007) evaluated the impact of the space-time structure of the rainfall on the distributed hydrological response and suggested that flash flood events were primarily controlled by the space-time structure of the rainfall. The entire circulation of water in a basin is governed by the spatial and temporal distribution of rainfall. Hence, it is crucial to quantitatively characterize the variability and the structure of intense precipitation in rainfall forecasting, flood warning, and real-time operation of major hydrosystem infrastructures to mitigate potential threats and losses caused by floods.

Although ground measurements of rainfall at raingauge are more accurate, radar measurements have gained increasing attention and become an essential source of the rain-field information because they can provide rainfall data with high spatio-temporal resolution (Smith *et al.* 2004; Viglione *et al.* 2010; Li *et al.* 2013; Finsen *et al.* 2014; Adjei *et al.* 2015). Quite a number of works have been carried out to analyze the structure of precipitation based on radar rainfall observations (Austin & Houze Jr 1972; Crane 1990; Steiner *et al.* 1995; Gebremichael & Krajewski 2004; Wu *et al.* 2015).

In this study, a geostatistical view of the precipitation field is adopted. Originally for mining, geostatistics is preferred because it offers a useful theoretical and mathematical description of spatially structural properties of natural phenomena and a practical technique to solve estimation problems (Berne *et al.* 2004). The geostatistics framework has also been applied in water sciences (Hevesi *et al.* 1992; Bacchi & Kottegoda 1995; Prudhomme & Reed 1999; Goovaerts 2000; Lloyd 2005; Buytaert *et al.* 2006; Skøien & Blöschl 2006). To quantify the variability of precipitation, Barancourt *et al.* (1992) addressed the issue of spatial intermittence of rainfall by developing a geostatistical model using a binary random function to describe the intermittency and, a second random function to represent the inner variability of rainfall inside the rainy areas. The procedure showed its clear superiority for delineating and estimating rainfall fields as compared with a classic global kriging. However, a procedure such as this has certain drawbacks: (1) independence between within-storm variability and variability due to fractional coverage must be assumed; (2) estimation variance cannot be produced; and (3) it is difficult to identify exactly what conditional estimates are sought and the impacts of independence assumption on the estimation due to the lack of mathematical precision of the estimation procedure.

Spatial variation of alpine precipitation was quantified by Germann & Joss (2001) by means of variogram analysis using high-resolution radar reflectivity data. Even under the difficult conditions in a mountainous region, the results gave quantitative answers to practical questions related to the spatial continuity. Berne *et al.* (2004) estimated the minimum resolutions of rainfall required for hydrological applications, based on quantitative investigations of the space-time scales of urban catchments and rainfall. The approach was proven to be relevant for various regions. Using the variogram within the geostatistics framework, the space-time structure of rainfall was studied. Berne *et al.* (2009) analyzed the variability of the spatial structure during intense Mediterranean precipitation using the concept of mean length, which was shown to be an efficient tool to represent the spatio-temporal variation of rain-fields. However, the indicator variogram, which could provide additional information about the structure and the correlation of the studied random field, was not used. Owing to the complexity of the spatial structure of precipitation fields, the identification of the range of a variogram remains a difficult task.

The main objective of this paper is to contribute to a better description of the dynamic time-space evolution of the rainfall during rainstorm events by combining the indicator variogram with the mean length. The paper is organized as follows. First, a brief description of the study area and the data preparation is presented. Then, the methodology to quantify the structure of rainfall is introduced. After discussions of the results, the conclusions that can be drawn from this study are presented.

## STUDY AREA AND DATA PREPARATION

### Study area

Hong Kong, with a population of about seven million people, is situated on China's south coast and is enclosed by the Pearl River Delta and South China Sea. Heavy rain in summer in Hong Kong is typically associated with the southwest monsoon and tropical cyclones. The threat of flooding is greatest during storm surges generated by the passage of typhoons due to high wind. Many parts of the Territory are densely populated urban areas surrounded by or situated within catchments that are typically small with relatively steep slopes. These urban areas and catchments have a relatively short time-of-concentration and are particularly susceptible to the threat of flash floods and extensive flooding rendering significant economic losses and possible fatalities. Apart from urban flash flooding, another disaster caused by persistent heavy rain in Hong Kong is landslides because of the hilly terrain.

### Ground rainfall data and radar rainfall data

*Z*in linear units mm

^{6}/mm

^{3}) to rainfall intensity

*R*in mm/h, the standard Marshall–Palmer relationship ( with and ) is used in many operational nowcasting systems. However, it is well-known that many factors can affect the accuracy of the radar-rainfall estimation and this relationship is too generalized, which may not be suitable in many cases. Another fact is that the relationship changes with time as the precipitation system evolves. SWIRLS makes use of both radar and raingauge data over Hong Kong to calibrate radar reflectivity in real-time for a reasonable relationship.

*b*in the relationship between radar–raingauge pairs, linear least square analysis is used. where is the radar reflectivity expressed in decibel;

*a*and

*b*are parameters of relationship; and is the ground rainfall expressed in decibels. All the reporting radar–raingauge pairs once accepted will be retained for the linear least square analysis throughout the entire rainstorm episode to ensure statistical significance.

^{2}) and temporal (6 min) resolution which is detected at 1 km height is correlated every 5 min with the rainfall recorded by the raingauges underneath to gain the optimal parameter

*a*and

*b*. Owing to the existence of winds, raindrops may deviate horizontally from their starting positions, so a certain adjusted approach of searching area from each raingauge position is devised and the radar image with low altitude is chosen to make sure the raindrops preserve their volume when they reach the ground. If there is no ground true value available as the rain has not fallen over any of the raingauges, such as a rainstorm is still outside Hong Kong, either the standard Marshall–Palmer relationship or the latest relationship will be used as first guess. As more radar–raingauge pairs are available, the relationship will be updated accordingly. Analysis strategies are also proposed to deal with the non-synchronous problem arising from the 6 min radar volume scans and the 5 min ground raingauges distributed over the Territory of Hong Kong (Li 2000). For a 6 min radar sweep, the radar data approximately corresponds to two 5 min raingauge observations and the apportioning of weights between the two latest available raingauge observations is specified when applying temporal interpolation. Figure 2 shows the approaches adopted to circumvent the non-synchronous problem and adjust the relationship.

### General features of four rainstorm events

In this study, an area of 64 × 64 km^{2} region covering the entire Territory of Hong Kong is considered. Four rainstorm events were chosen.

#### 2007-05-18 and 2007-05-19 rainstorm events

On 18 May 2007, a trough of low pressure developed over inland Guangdong and moved across the south China coast. A squall line swept across Hong Kong from northwest to southeast that evening, bringing heavy showers and severe gusts to the Territory. A peak gust over 100 km/h was recorded at Waglan Island. With the trough of low pressure lingering along the south China coast, there were heavy showers and thunderstorms between 19 and 22 May.

#### 2008-04-19 rainstorm event

Under the combined effect of Typhoon Neoguri and the northeast monsoon, local winds started to pick up on 18 April 2008. Local winds became generally strong on the afternoon of 19 April 2008 when Neoguri was about 200 kilometers to the west-southwest of Hong Kong. When Neoguri approached the coast of western Guangdong, the warm southerly winds associated with Neoguri met the relatively cooler northeast monsoon and formed a warm front with severe convective activities over the coastal waters of Guangdong. The warm front moved from south to north across the coast of Guangdong and brought heavy rain to Hong Kong on that day. The total daily rainfall recorded at the HKO on that day was 233.4 mm, the highest daily rainfall amount recorded in April since records began. After making landfall and moving further inland, Neoguri weakened rapidly. Locally, rain also eased off rapidly with just a few showers on 20 April 2008.

#### 2009-09-15 rainstorm event

A tropical depression over the western North Pacific entered the northern part of the South China Sea on 13 September 2009. It intensified into a tropical storm that evening and was named Koppu. The outer rainbands of Koppu brought a few thundery showers to Hong Kong during that evening. Koppu intensified into a typhoon on 14 September and the weather became cloudy with squally showers. Local winds also strengthened gradually towards the evening. Gale force southeasterly winds with maximum gusts up to 151 km/h were recorded at the Cheung Chau Beach in the late evening of 14 September. Koppu made landfall over the western coast of Guangdong on the morning of 15 September and weakened into a tropical storm in the afternoon. The rainbands associated with Koppu brought heavy squally showers to the Territory on that day. With Koppu moving further inland and dissipating, the showers gradually eased off on 16 September.

For the purposes of illustration, the rainstorm that occurred on 19 April 2008 is used herein.

## METHODOLOGY

### Theoretical variogram model

*R*is the random variable under consideration (e.g., rainfall intensity). The semi-variogram does not depend on the mean of the random function, therefore is more robust than the covariance.

Isotropic variogram describes a random field in which spatial correlation does not vary with directions but only on the separation distance. It is then a function of the modulus of the vector . When the variogram shows different behavior along different directions, the random field is anisotropic.

*et al.*1992). However, the distribution of rain rates is significantly asymmetric and skewed toward high values and hence far from normality at short accumulation periods. A simpler answer to circumvent the non-Gaussian distribution issue is by thresholding which offers an application of the indicator method to map the probability distributions of rainfall (Steffens 1987). In the classical approach, the rainfall process is analyzed as a random field with being a non-negative value of rainfall rate (or amount) that fell at location

*x*at time

*t*during event

*w*. In this case, the actual rain process is transformed into a binary process to distinguish whether the rainfall intensity at location

*x*at time

*t*is above a given threshold

*k*under consideration. For this, a binary function denoted is defined by: The indicator function will be if the rainfall intensity is above a given threshold

*k*. The indicator variograms of the rain-field for each threshold will be calculated based on these indicator values . These indicator variograms can provide useful information about the spatial intermittency of the rain-field for the considered thresholds as well as the size and shape of the rainy areas above/below the thresholds.

### Fitting the theoretical variogram model to experimental data

To estimate nugget effect, sill, and range for each sample indicator variogram, it is necessary to fit a model to the experimental variogram. Some of the models that are often used in practice include linear, spherical, exponential and Gaussian variogram models.

*t*and direction , , by minimizing where is the total number of considered distance lags. From the visual inspection of the indicator variograms, nugget effects are negligible for most directions and time instants, thus is set to 0 during the fitting procedure. In most cases, variogram value increases with distance but there is an erratic behavior in some directions when distance lag between pixels is large. Hence, high weights to the small distances are given by the weighted least squares technique (Cressie 1985) in this study to determine optimal variogram model parameters as: where the weights is given by . The distance bin that has the maximum number of pairs is about 25 km in the majority of the rainfall intensity thresholds and time instants considered. Thus, distance separation less than or equal to 50 km is considered in the process of fitting variogram models in attempting to identify the best-fit variogram model for further analysis.

### Mean length

*t*during a rainstorm event

*w*above the threshold in a given direction ; is the proportion of rainfall intensity values above the threshold

*k*in the direction ; and is the indicator variogram associated with the rainfall threshold

*k*in the direction .

Analysis of the sample indicator variograms in many directions suggests that they are linearly increasing for short distance lag from 1 to 9 km. Therefore, the derivative of in Equation (7) is estimated as the slope of the regression line between the sample indicator variogram values and distance lag from 1 to 9 km. Although only the points within 9 km are considered in the calculation of the derivative of the variogram which may not be as reliable as using all the data, by limiting calculations to sufficiently short distance lags makes the simple linear model become valid. In addition, only local stationarity is required to estimate the indicator variogram considering short distance lags (Berne *et al.* 2009). Furthermore, this linearity assumption is also confirmed by the high correlation coefficients (which measures the strength of linear dependence) between the sample data from 1 to 9 km.

The domain size that is rainy must be suitable to the mean length calculation. The sample variogram and the mean proportion are representative of the rain-field only if the domain is large enough and appropriately located to observe the entire precipitating system (Berne *et al.* 2009). Based on that, mean length can be derived. In addition, a proportion above a given threshold close to 1 means that the entire study domain is rainy above the threshold whereas a proportion above a given threshold close to 0 means that there is nearly no rainfall above the threshold within the studied area. Hence, in this study, the mean length of the rain-field is not calculated if the proportion of area where rainfall intensity is above the given threshold is higher than 99% or lower than 1%.

Range of the indicator variogram and mean length are two different characteristic scales of a random function, and both of them offer important information about the spatial structure of rain-field. Range is the limiting distance beyond which two points are uncorrelated, which means that within the range rainfall intensities at two points have some correlation. Mean length is the average length of the segments defined by the rainfall intensity value above the considered threshold, which means, on average, two points separated by a distance that is less than the mean length tend to belong to the same category (above or below the considered threshold). It is interesting to investigate the relationship between these two since mean length has been proved to be an efficient measure to represent the variability of the spatial structure of rain-field by Berne *et al.* (2009). In this study the mean length is used to check the automatic fitting procedure of indicator variogram, to study its correlation with range, and to characterize the evolution of spatial structure of rain-field for the four studied rainstorm events along with the range.

## RESULTS AND DISCUSSION

### Spatial structure of rain-field

. | Rain rate quantile levels . | ||||
---|---|---|---|---|---|

Event . | 10% . | 30% . | 50% . | 70% . | 90% . |

2007-05-18 | 0.036 | 1.035 | 1.914 | 2.928 | 10.813 |

2007-05-19 | 1.112 | 2.239 | 3.373 | 5.285 | 11.66 |

2008-04-19 | 0.827 | 2.047 | 3.756 | 7.135 | 16.552 |

2009-09-15 | 0.078 | 1.19 | 2.735 | 5.545 | 13.03 |

. | Rain rate quantile levels . | ||||
---|---|---|---|---|---|

Event . | 10% . | 30% . | 50% . | 70% . | 90% . |

2007-05-18 | 0.036 | 1.035 | 1.914 | 2.928 | 10.813 |

2007-05-19 | 1.112 | 2.239 | 3.373 | 5.285 | 11.66 |

2008-04-19 | 0.827 | 2.047 | 3.756 | 7.135 | 16.552 |

2009-09-15 | 0.078 | 1.19 | 2.735 | 5.545 | 13.03 |

The indicator maps for different threshold *k* at different time during event are plotted and indicator variograms for each indicator map are calculated the same way as standard variograms, except that the indicator values are used in place of the actual rainfall intensity values. The analysis result of the rainstorm that occurred on 19 April 2008 is shown herein to illustrate the method.

Distance separation greater than 50 km is not included in the fitting procedure to avoid the erratic behavior of the variogram in some direction when distance lag gets large. Among the four theoretical variogram models, the exponential variogram was found to best fit the sample variograms (see example results in Table 2) in the majority of the rainfall intensity thresholds and time instants considered with the highest mean R^{2} = 0.928 (0.905 for spherical variogram, 0.886 for Gaussian variogram and 0.834 for linear variogram, respectively).

. | Threshold = 2 mm/h . | Threshold = 10 mm/h . | ||||
---|---|---|---|---|---|---|

Angle (°) . | Range (km) . | Sill . | Coefficient of determination R^{2}
. | Range (km) . | Sill . | Coefficient of determination R^{2}
. |

−80.54 | 138.33 | 0.36 | 0.986 | 48.48 | 0.14 | 0.954 |

−71.57 | 116.63 | 0.3 | 0.988 | 45.99 | 0.15 | 0.895 |

−63.43 | 85.56 | 0.24 | 0.984 | 57.36 | 0.17 | 0.91 |

−56.31 | 59.57 | 0.19 | 0.964 | 69.25 | 0.2 | 0.929 |

−50.19 | 48.44 | 0.16 | 0.92 | 81.06 | 0.22 | 0.94 |

−45 | 33.58 | 0.14 | 0.951 | 77.95 | 0.23 | 0.941 |

−39.81 | 20.91 | 0.12 | 0.885 | 56.34 | 0.21 | 0.889 |

−33.69 | 30.96 | 0.13 | 0.885 | 65.08 | 0.22 | 0.919 |

−26.57 | 25.96 | 0.12 | 0.876 | 50.62 | 0.2 | 0.895 |

−18.43 | 29.15 | 0.13 | 0.841 | 39.98 | 0.19 | 0.875 |

−9.46 | 40.98 | 0.14 | 0.86 | 35.17 | 0.17 | 0.878 |

0 | 45.29 | 0.16 | 0.883 | 28.99 | 0.17 | 0.863 |

9.46 | 116.81 | 0.26 | 0.928 | 33.52 | 0.17 | 0.901 |

18.43 | 170.39 | 0.37 | 0.945 | 34.82 | 0.18 | 0.892 |

26.57 | 227.3 | 0.49 | 0.955 | 37.64 | 0.2 | 0.892 |

33.69 | 256.85 | 0.58 | 0.955 | 45.23 | 0.22 | 0.907 |

39.81 | 327.85 | 0.71 | 0.961 | 55.5 | 0.23 | 0.928 |

45 | 377.84 | 0.79 | 0.953 | 47.8 | 0.23 | 0.908 |

50.19 | 237.67 | 0.6 | 0.954 | 66.47 | 0.24 | 0.928 |

56.31 | 326.44 | 0.72 | 0.963 | 61.54 | 0.23 | 0.932 |

63.43 | 244.26 | 0.58 | 0.972 | 55.03 | 0.22 | 0.918 |

71.57 | 221.23 | 0.54 | 0.985 | 53.27 | 0.2 | 0.918 |

80.54 | 217.19 | 0.53 | 0.985 | 49.62 | 0.18 | 0.903 |

90 | 188.13 | 0.46 | 0.985 | 33.76 | 0.15 | 0.836 |

. | Threshold = 2 mm/h . | Threshold = 10 mm/h . | ||||
---|---|---|---|---|---|---|

Angle (°) . | Range (km) . | Sill . | Coefficient of determination R^{2}
. | Range (km) . | Sill . | Coefficient of determination R^{2}
. |

−80.54 | 138.33 | 0.36 | 0.986 | 48.48 | 0.14 | 0.954 |

−71.57 | 116.63 | 0.3 | 0.988 | 45.99 | 0.15 | 0.895 |

−63.43 | 85.56 | 0.24 | 0.984 | 57.36 | 0.17 | 0.91 |

−56.31 | 59.57 | 0.19 | 0.964 | 69.25 | 0.2 | 0.929 |

−50.19 | 48.44 | 0.16 | 0.92 | 81.06 | 0.22 | 0.94 |

−45 | 33.58 | 0.14 | 0.951 | 77.95 | 0.23 | 0.941 |

−39.81 | 20.91 | 0.12 | 0.885 | 56.34 | 0.21 | 0.889 |

−33.69 | 30.96 | 0.13 | 0.885 | 65.08 | 0.22 | 0.919 |

−26.57 | 25.96 | 0.12 | 0.876 | 50.62 | 0.2 | 0.895 |

−18.43 | 29.15 | 0.13 | 0.841 | 39.98 | 0.19 | 0.875 |

−9.46 | 40.98 | 0.14 | 0.86 | 35.17 | 0.17 | 0.878 |

0 | 45.29 | 0.16 | 0.883 | 28.99 | 0.17 | 0.863 |

9.46 | 116.81 | 0.26 | 0.928 | 33.52 | 0.17 | 0.901 |

18.43 | 170.39 | 0.37 | 0.945 | 34.82 | 0.18 | 0.892 |

26.57 | 227.3 | 0.49 | 0.955 | 37.64 | 0.2 | 0.892 |

33.69 | 256.85 | 0.58 | 0.955 | 45.23 | 0.22 | 0.907 |

39.81 | 327.85 | 0.71 | 0.961 | 55.5 | 0.23 | 0.928 |

45 | 377.84 | 0.79 | 0.953 | 47.8 | 0.23 | 0.908 |

50.19 | 237.67 | 0.6 | 0.954 | 66.47 | 0.24 | 0.928 |

56.31 | 326.44 | 0.72 | 0.963 | 61.54 | 0.23 | 0.932 |

63.43 | 244.26 | 0.58 | 0.972 | 55.03 | 0.22 | 0.918 |

71.57 | 221.23 | 0.54 | 0.985 | 53.27 | 0.2 | 0.918 |

80.54 | 217.19 | 0.53 | 0.985 | 49.62 | 0.18 | 0.903 |

90 | 188.13 | 0.46 | 0.985 | 33.76 | 0.15 | 0.836 |

Estimated ranges for the threshold of 2 mm/h and 10 mm/h in different directions indicate that the shapes of the rain-fields as well as the magnitude of the ranges are different for the two considered thresholds. For the threshold of 2 mm/h, large ranges exist in the northeast–southwest direction and ranges are comparatively small along the northwest–southeast direction. While for the threshold of 10 mm/h, relatively larger ranges can be found in both northeast–southwest and northwest–southeast directions. The value of the maximum range for the threshold of 10 mm/h is about 80 km, which is much smaller than the maximum value (400 km) for the threshold of 2 mm/h. For each time step, the spatial structure of rain cells above the considered threshold more or less exhibits an elliptic shape just like these two examples shown. Therefore, it is possible and sufficient to describe the shape of the rain-field by the values and the directions (quantified as an angle) of the maximum range and the minimum range instead of the large amount of information (ranges and sills for 24 different directions) of the spatial structure at each time step.

### Relationship between variogram range and mean length

It is interesting to investigate the behavior of range and mean length in relation to time. There are some features that can be observed. First, maximum range and maximum mean length share a similar trend, while the angle of the maximum range may not be identical to that of the maximum mean length for some time instants. According to rain-field measurements, it is not surprising to observe the above-mentioned features because: (1) although the angle of the maximum range and the angle of the maximum mean length are different, the values are very close, so are the values of maximum range and maximum mean length; (2) when the spatial structure of the rain-field displays more or less a circular shape, the two angles may differ a lot but the values of maximum range and maximum mean length are similar; (3) mean lengths of a category representing the rain cells above the threshold *k*, where the corresponding , can be readily calculated from continuous data as the total length of in the direction divided by the total number of embedded occurrences of in the direction . When multiple embedded occurrences of exist in some direction , mean length of this direction will be much smaller than the range which is not affected that much by the number of the embedded occurrences of .

Rainstorm event . | 2007-05-18 . | 2007-05-19 . | 2008-04-19 . | 2009-09-15 . |
---|---|---|---|---|

Threshold between quantile level 10–30% | 0.7561 | 0.6707 | 0.7437 | 0.7541 |

Threshold between quantile level 70–90% | 0.8391 | 0.7504 | 0.5471 | 0.783 |

Rainstorm event . | 2007-05-18 . | 2007-05-19 . | 2008-04-19 . | 2009-09-15 . |
---|---|---|---|---|

Threshold between quantile level 10–30% | 0.7561 | 0.6707 | 0.7437 | 0.7541 |

Threshold between quantile level 70–90% | 0.8391 | 0.7504 | 0.5471 | 0.783 |

Second, it is difficult to identify the periodicity of spatial structure parameters for the 2008-04-19 rainstorm event. However, the peaks of the maximum range, maximum mean length, minimum-to-maximum range ratio, and minimum-to-maximum mean length ratio exist for the 2007-05-18 rainstorm event with a periodicity of about 3 hours which is not shown in this paper. The general feature for all considered rainstorm events is the negative correlation between the maximum range (mean length) and the minimum-to-maximum range (mean length) ratio for both thresholds, which indicates that the spatial structure of the rain-field is stretched for the large maximum range and mean length, but circular for small maximum range and mean length.

## CONCLUSIONS

During a rainstorm, the precipitation intensity is highly variable in time and space. Rainfall data with high space-time resolution collected by radar have recently been used more frequently as inputs for distributed hydrological modeling of floods, erosion, and other processes.

In this paper, a geostatistical approach was adopted to analyze the variability of the spatial structure of the rain-field. Four rainstorm events that occurred in 2007, 2008, and 2009 in Hong Kong were used to illustrate the method. Indicator variograms of rain-fields had been examined which revealed substantial anisotropy for all rainfall thresholds considered. Based on indicator variograms, the ranges and mean lengths above different thresholds in 24 directions were estimated for each 6 min time step.

The conclusions that could be drawn from the study of spatial structures of observed rainfall in Hong Kong are listed below:

The behavior of variograms is not regular with large distance in some directions. Higher weights to the small distances should be given and distances less than or equal to 50 km are considered when fitting the variogram model.

The spatial structure of rain-field for the four rainstorm events is affected by strong anisotropy. The calculation of range and mean length in different directions is needed to capture the spatial structure of anisotropic rain-fields. The influence of this anisotropy condition on generating rain-fields according to the variogram should be investigated.

The spatial structure of the four chosen rainstorm events exhibits a more or less elliptic shape. Therefore, it is possible and sufficient to describe the shape of the rain-field by the values and the directions (quantified as an angle) of the maximum range and the minimum range instead of the large amount of information (ranges and sills for 24 different directions) of the spatial structure at each time step. The negative correlation between the maximum range (mean length) and the minimum-to-maximum range (mean length) ratio for both thresholds can be identified for all considered rainstorm events, which indicates that the spatial structure of the rain-field is stretched for the large maximum range and mean length, but circular for small maximum range and mean length.

The values of correlation coefficients between the maximum (minimum) range and maximum (minimum) mean length for the selected rainstorm events give useful information about the spatial structure of the rain-field. When multiple rainstorm centers above the considered threshold exist, the correlation between range and mean length of the corresponding rainstorm event becomes lower.

## ACKNOWLEDGEMENTS

The authors would like to thank the two anonymous reviewers and the editor who helped us improving the quality of the original manuscript. The authors wish to acknowledge the support of the Hong Kong Research Grant Council (Project no. 620110: Development of time-space rainstorm model for Hong Kong) and Nanjing Hydraulic Research Institute (Project no. Y515014) for the study. Gratitude is extended to the Hong Kong Observatory for providing the rainfall radar data used in the study.