1.Nansen-Zhu International Research Center, Institute of Atmospheric Physics, Chinese Academy of Sciences, Beijing 100029, China. 2.University of Chinese Academy of Sciences, Beijing 100029, China Manuscript received: 2021-01-21 Manuscript revised: 2021-05-25 Manuscript accepted: 2021-05-28 Abstract:Land surface temperature (LST) is one of the most important factors in the land-atmosphere interaction process. Raw measured LSTs may contain biases due to instrument replacement, changes in recording procedures, and other non-climatic factors. This study attempts to reduce the above biases in raw daily measurements and achieves a homogenized daily LST dataset over China using 2360 stations from 1960 through 2017. The high-quality land surface air temperature (LSAT) dataset is used to correct the LST warming biases especially evident during cold months in regions north of 40oN due to the replacement of observation instruments around 2004. Subsequently, the Multiple Analysis of Series for Homogenization (MASH) method is adopted to detect and then adjust the daily observed LST records. In total, 3.68 × 103 effective breakpoints in 1.65 × 106 monthly records (about 20%) are detected. A large number of these effective breakpoints are located over large parts of the Sichuan Basin and southern China. After the MASH procedure, LSTs at more than 80% of the breakpoints are adjusted within +/– 0.5oC, and of the remaining breakpoints, only 10% are adjusted over 1.5oC. Compared to the raw LST dataset over the whole domain, the homogenization significantly reduces the mean LST magnitude and its interannual variability as well as its linear trend at most stations. Finally, we perform preliminary analysis upon the homogenized LST and find that the annual mean LST averaged across China shows a significant warming trend [0.22oC (10 yr)–1]. The homogenized LST dataset can be further adapted for a variety of applications (e.g., model evaluation and extreme event characterization). Keywords: land surface temperature (LST), daily observation, homogenization, MASH method, variability 摘要:地表土壤温度是陆-气相互作用过程中的重要因素之一。观测的地表土壤温度数据易受台站迁移、仪器更换、记录方式变更以及观测站周边环境改变等非气候因素的影响,从而产生不同程度的偏差。这种由非气候因素造成的变化统称为时间序列的非均一性。依据这样的非均一化序列得出的研究结果,极有可能会对序列的长期线性趋势以及极端气候事件的评估产生偏差,弱化真实气候变化的影响,甚至得到与真实变化相反的结论。因此,本文的研究工作主要是将中国2360个气象观测站点1960~2017年的逐日地表土壤温度数据进行均一化处理,尽可能地减少地表土壤温度数据的非均一性偏差。我们首先利用质量较高的观测气温数据修正了地表土壤温度自2005年起北纬40o以北地区冷月份出现的暖偏差现象。随后,应用多元均一化方法(MASH)对逐日地表土壤温度数据的非均一性进行检测和校订。总的来说,在1.65 × 106个月均记录中,共检测出3.68 × 103个有效断点记录(约占总数的20%),有效断点记录较多的站点主要分布在四川盆地地区以及中国南方的大部分地区。通过MASH方法调整之后,地表土壤温度序列有超过80%的偏差调整分布在+/– 0.5oC之间,只有10%的偏差调整大小超过1.5oC。我们将均一化后与原始的观测地表土壤温度数据进行比较,发现均一化过程显著降低了大部分站点地表土壤温度的平均量级、年际变率以及线性趋势。最后,我们还对均一化的地表土壤温度进行了初步分析,结果表明近年来中国年均地表土壤温度呈显著的增温趋势[0.22oC (10 yr)–1]。本文的均一化逐日地表土壤温度的观测数据集今后可进一步为各科学研究应用提供可靠的数据支撑(例如:模型评估和极端事件表征等)。 关键词:地表土壤温度(LST), 逐日观测, 均一化, 多元均一化(MASH)方法, 变率
HTML
--> --> --> -->
2.1. In situ observed LST
The raw daily LST dataset from meteorological stations in China, spanning the period 1960?2017, was obtained from the National Meteorological Information Center of the China Meteorological Administration (NMIC/CMA). Fundamental quality control (e.g., screening for unreasonable extreme values) was performed on this dataset before it was released to the public (http://data.cma.cn/data). In China, a large number of meteorological stations were established in the early 1950s, and the station density and records were maintained with relatively high continuity and stability after 1960 (Shi et al., 2014; Cao et al., 2016). Currently, more than 2400 national meteorological stations exist in the mainland of China. Land surface temperature is one of the factors regularly measured and collected every day at the meteorological stations. Before 2000, LST was recorded and stored manually four times a day (at 0200, 0800, 1400, and 2000 Beijing time, Beijing time=UTC+8) with a surface and bent stem earth mercurial thermometer. After 2000, the observation system was updated gradually to employ a platinum resistance temperature sensor, which is an automatic instrument and is more effective than mercurial thermometers. After the update, the observation frequency became hourly (twenty-four times a day, Ren et al., 2013). The renewal period is concentrated during 2000?07 across the mainland of China, and the observation systems north of 40oN were updated in 2004 [see Fig. 1 of Xu et al. (2019)]. The arithmetic average of the observations collected at multiple times within a day is regarded as the daily LST in the data collection. Liu et al. (2008) compared differences between automatic and manual observed LSTs in daily, monthly, and annual scales during the parallel observation period and found that the substantial differences mainly appear in snow-covered regions, e.g., northern Heilongjiang, northern Inner Mongolia, and most of Xinjiang provinces. In Southern China, the observed differences between the two instruments are very small. In the present work, daily LST measurements from up to 2360 meteorological stations are used. The majority of stations are located in relatively low elevation regions, which are usually densely populated (Fig. 1a). For example, there is a much higher density of stations in the Yellow River and Yangtze River basins, Southeast China, and the Central China Plain compared to other regions. The station distribution is relatively sparse in high elevations and sparsely populated areas, such as Northwest China and the Qinghai-Tibet Plateau regions. In addition, the number of effective stations (i.e., stations with measurements) was 1476 in 1960, after which it increased generally over time (stable during 1980?2010). In 2017 the number of effective stations increased to 2628 (Fig. 1b).
2 2.2. Multiple Analysis of Series for Homogenization (MASH) -->
2.2. Multiple Analysis of Series for Homogenization (MASH)
The MASH method was developed by Szentimrey (1999, 2014) and is based on the hypothesis test method to detect possible breakpoints at a given significance level. Through comparisons of measurements at different stations within the same climate region, the MASH method does not require prior assumptions of a homogeneous time series. This method has been widely applied to detect and adjust the inhomogeneity of raw meteorological observations at ground stations (e.g., Li et al., 2018, 2020). Guijarro et al. (2017) tested nine commonly used homogenization methods (including the RHtest and MASH methods) and compared their homogenized performances in terms of the root mean square errors and trends of the air temperature time series. They found that the results obtained by MASH method were comparatively reliable (Guijarro et al., 2017). To homogenize daily records, the MASH method must first homogenize the corresponding monthly data. Therefore, the daily LST at each station is first aggregated to monthly values, and then, the breakpoints of the monthly LST are detected and adjusted. Finally, the MASH method is again applied to homogenize the daily LST with the incorporation of the homogenized monthly values. Detailed information of the MASH method, including the mathematics it uses and its technique, is provided in its online manual (https://www.met.hu/en/omsz/rendezvenyek/homogenization_and_interpolation/software/). The latest version of MASH, v3.03, is used in this study. According to the description in the MASH manual, two different models can be selected and used. One is the additive model, which requires that the targeted dataset has a normal distribution (e.g., temperature). The other is the multiplicative model and can be used for a quasi-lognormally distributed data series (e.g., precipitation). Moreover, the Monte Carlo method is used in MASH to detect the inhomogeneity of time series with its threshold of precision (0.1, 0.05, or 0.01). In general, the smaller the Monte Carlo’s threshold is, the more stringent the detection of inhomogeneity will be (Szentimrey, 2014). Using different thresholds might reduce the number of breakpoints, but the frequency distribution patterns of breakpoints are similar (figures not shown). In this study, we choose the additive model and define a Monte Carlo threshold of 0.05 as the significance level. In the original MASH procedure, the monthly/annual value is set as missing if any missing day/month exists within that month/year. Such a strict criterion will lead to the loss of many useful records because many stations only have few days missing in a specific month. Furthermore, the loss of useful data is not the intention of data homogenization. Here, we use a lenient threshold condition for the missing value judgment to retain as many useful observation stations as possible. At each station, the monthly LST is set as a missing value when more than nine days of daily LST is missing in a given month. We also investigated the impact of different criteria (i.e., 8, 9, 10 days missing) for the count of missing months and found that there is little difference when varying criteria for a 28, 29, 30, and 31 day month. Meanwhile, the annual LST is set as a missing value when more than three continuous monthly values are missing. Finally, we remove stations with available annual values totaling less than 30 years of the full 58 years. Eventually, 2360 stations remained and were homogenized by the MASH method (shown as the straight solid line in Fig. 1b). According to the principle of MASH as well as the spatial variability of LST, we perform MASH in each individual climate region. Based on the natural conditions for agricultural production and also in consideration of climate characteristics, we divide the mainland of China into nine subregions (Fig. 1a): the Huanghe-Huaihe-Haihe Plain (HHH), Loess Plateau (LP), Middle-lower Yangtze Plain (YZ), Northeast China Plain (NE), Northern arid and semiarid region (NA), Qinghai-Tibet Plateau (TB), Sichuan Basin and surrounding regions (SC), South China (SE), and the Yunnan-Guizhou Plateau (YG). The shapefile of each subregion is available from the Institute of Geographical Sciences and Resources, Chinese Academy of Sciences (http://www.resdc.cn/data.aspx?DATAID=275), and the number of effective stations in each subregion is shown in Table 1.
Full name
Abbreviation
Number of stations
Huanghe-Huaihe-Haihe Plain
HHH
414
Loess Plateau
LP
202
Middle-lower Yangtze Plain
YZ
488
Northeast China Plain
NE
183
Northern arid and semiarid region
NA
328
Qinghai-Tibet Plateau
TB
90
Sichuan Basin and surrounding regions
SC
200
South China
SE
164
Yunnan-Guizhou Plateau
YG
291
Mainland of China
China
2360
Table1. Number of stations in each subregion
In addition, other statistical methods, including linear regression and standard deviation, are used to comparatively analyze the raw and homogenized LST dataset. A two-tailed Student’s test is used to test the significance of these statistics.
-->
3.1. Preliminary adjustment of LSTs in northern China
As mentioned in the introduction section, automatic instruments for LST measurements began to replace manual ones in 2004 in northern China (mainly north of 40oN, including Xinjiang Province, NE, and NA subregions, shown as black dots in Fig. 1a), which resulted in LSTs increasing abruptly in cold months since 2005. To understand this result, we select one cold month (December) as an example to analyze the time series of LST over northern China. Figure 2 shows the daily LST time series averaged across 197 stations in northern China in December from 1960 to 2017. There is a distinct jump in 2005, after which the magnitude of LST increases remarkably. The mean value is –8.1oC for 2005?17, which is 8oC higher than that for 1960?2005 (–16.1oC). This phenomenon is prevalent at all 197 stations. Xu et al. (2019) found a similar problem in the same regions (the NE and NA subregions) when they compared the differences of LST measurements from manual and automatic instruments during parallel observation periods. The warm shift phenomenon is principally caused by the change of the observation system from a manual to an automatic one around 2004. In winter, when the ground surface is covered by snow, the manual instrument measures the temperature at the snow surface, whereas the automatic instrument sensor measures the temperature at the soil surface under snow. Because snow is a strong insulator of heat, it can absorb both longwave radiation from the ground surface transmitted upward and shortwave radiation from the atmosphere transmitted downward (Cohen and Rind, 1991; Groisman et al., 1994). Therefore, the measured LST from the automatic instrument would change much more slowly under snow and cannot represent real LST change features (Liu et al., 2008; Ren et al., 2013). When the manual sensor was buried in snow, it would be taken out to measure the snow surface temperature instead of the soil surface temperature (China Meteorological Administration 2003). Figure2. Time series of the raw daily LST averaged across 197 stations (the black dots in Fig. 1a) in December for 1960?2017. The red solid line is a reference line to separate the years before and after 2005; the two blue dotted lines are the mean LSTs derived from the raw daily dataset during 1960?2005 and 2005?17. The green solid curve represents the daily LST time series after LSAT adjustments (section 3.1), and the red dotted line is the mean LST during 2005?17. The corresponding mean LST values averaged for different periods are also indicated.
More specifically, we take a station (ID 50862, 46.98oN, 128.05oE) at the NE subregion as an illustrative example. Figure 3 shows the abrupt warming shift in cold months (from October to the following April) since 2005. A similar phenomenon appears at all 197 stations (black dots in Fig. 1a) in the NE and NA subregions. In the MASH procedure, possible breakpoints are determined by comparing the values at the candidate station with those at the nine nearest reference stations. If those surrounding reference stations show similarly abrupt changes or shifts as the candidate station, then the MASH method cannot detect them (Li, 2016). Due to how MASH works, it will fail to deal with the specific problematic phenomenon mentioned above (compare the blue and orange lines in Fig. 3b). Thus, before applying the MASH method, we perform a preprocessing procedure for the LSTs from these 197 stations. Figure3. Case station (ID 50862, 46.98oN, 128.05oE) for the raw and calculated LST, and the homogenized results (units: oC). (a) Raw daily LST plotted against the calculated daily LST in each month during 1960?2004, where the black solid line is the reference (x = y) line, (b) raw (blue) and MASH homogenized (orange) daily LST, and (c) raw and calculated (green line) LST during 2003?07. The calculated daily LST is the LST adjusted by the LSAT (described in section 3.1).
There is a very close relationship between the LSAT and LST, and their differences determine surface heat fluxes (Zeng et al., 2012). The observed LSATs have undergone a strict quality control process and do not show such remarkable warming shifts. Therefore, the LSAT is used as a reference to correct the LST warming bias at each station. Simplistically and practically, it is assumed that the characteristics of the changes in LSATs are consistent with those in LSTs at the same station. This assumption is reasonable because they have a robust relationship and show similar variabilities (Vancutsem et al., 2010). The following procedure is used to adjust the LST via the LSAT. First, we construct a regression equation between the LST (dependent variable) and LSAT (independent variable) for each cold month (from October to the following April) at each of the 197 stations from 1960 to 2004. Second, the regression coefficient and the raw daily LSAT in the current month are used to compute the corresponding daily LST from 2005 to 2017. The computed LSTs are regarded as the “calculated LSTs” at the 197 stations. To verify the reasonableness and applicability of the above hypothetical relationship, we compare the raw and calculated LSTs in Fig. 3a. All the dots spread around the reference y-x line, and the monthly absolute mean differences between the calculated and raw LSTs are generally less than 1oC. In cold months, the absolute differences are less than 0.5oC, except in April (October), when there is a relatively large error in the mean differences of approximately –2oC (2oC). However, the standard deviation of the raw LST during 1960?2005 in April (October) is 3oC (6oC) and is higher than the mean difference. Therefore, it still can be concluded that the calculated LSTs are consistent with the raw LSTs during the whole period. Similar results are also shown at other stations. After the above process, the distinct warm shift of the LST in cold months is removed (Fig. 3c). The calculated daily LST across all 197 stations averaged in December from 2005 to 2017 (green line in Fig. 2) also shows consistency with the raw daily LST from 1960 to 2005, and the mean value for 2005?17 (–15.9oC) is close to that for 1961?2005 (–16.1oC). The above-calculated LSTs at 197 stations for 2005?17 are added to the raw dataset and replace the values at the same time and station.
2 3.2. Breakpoint detection by MASH -->
3.2. Breakpoint detection by MASH
After the above preliminary adjustments, we apply the MASH method at all 2360 stations in China. The first step of MASH is to detect the temporal breakpoints of the LST time series at each station. The breakpoint (also called the change-point) is where the time series displays significant differences before and after that point. The time series shows a distinct leap at the breakpoint. To help understand this process, we take one station (ID 57710 at 27.85oN, 106.37oE) in the YG subregion as an illustrative example (Fig. 4). The LST at the candidate station (the red dot in Fig. 4a) is first compared with the values from the nine closest stations (the green dots in Fig. 4a). Compared with the other nine reference time series (Fig. 4b), a breakpoint appears in 1970 in the candidate time series, of which the mean LST during 1960?70 is 21.1oC, 3oC higher than that during 1970?2017 (18.1oC). The variability of the homogenized time series (the blue line in Fig. 4c) is akin to the nine neighbor reference time series. The time series has a warming trend [0.09oC (10 yr)–1], showing the opposite tendency compared to the raw time series [–0.26oC (10 yr)–1]. Figure4. Annual LST series at station ID 57710 (27.85oN, 106.37oE, a candidate station) in the YG subregion (units: oC). The specific information of nine reference stations is ID 57714 (27.36oN, 106.20oE), ID 57717 (27.68oN, 106.92oE), ID 57713 (27.68oN, 106.92oE), ID 57606 (28.33oN, 106.67oE), ID 57720 (27.95oN, 107.17oE), ID 57614 (28.55oN, 105.98oE), ID 57803 (27.05oN, 106.00oE), ID 57718 (27.03oN, 106.72oE), and ID 57719 (27.07oN, 106.97oE), respectively. (a) Distribution of stations, including the candidate station (red dot), the nine nearest reference stations (green dots), and other stations (black dots) in the YG subregion, (b) the raw annual LST anomalies of the candidate station (red curve) and the nine reference stations (black curves), and (c) annual LST from the raw (red curve) and homogenized time series at the candidate station.
Repeating the above procedure for all stations in each of the nine subregions, we identify the breakpoints at all 2360 stations from the monthly LST time series for 1960?2017. To better illustrate the results, we subjectively divided MASH results into two parts. The first part occurs when the absolute adjustment value is greater than 0.5oC, it is treated as the effective adjustment and its corresponding breakpoint as the effective breakpoint. The other part occurs when the absolute adjusted value is less than 0.5oC, it is regarded as the minor adjustment, in which inhomogeneity is relatively small and the MASH procedure has little effect on the time series. There are a total of 3.68 × 103 effective breakpoints counted in Fig. 5. The plot clearly shows that the monthly LSTs at the majority of stations contain 5?25 effective breakpoints (Fig. 5). Of all 2360 stations, 35 stations contain over 40 effective breakpoints, of which most are located in the SC and SE subregions (the red dots in Fig. 5a), while 21 stations scattered across China contain no effective breakpoints (the dark blue dots in Fig. 5a). The effective breakpoints are relatively concentrated in the SE, HHH, and SC subregions, where there are at least 20 effective breakpoints identified in most stations. Having aggregated the numbers of effective breakpoints at all stations (Fig. 5b), nearly 500 effective breakpoints occur each year on average. However, the number of effective breakpoints shows distinct interannual variations and evidently increases over time, in particular since 2000. In 2003, when the replacement of the LST measurement instruments occurred at many stations throughout China, more than 1200 effective breakpoints are identified. At this time, the number of effective breakpoints reaches its maximum value. For the monthly LST time series, the number of effective breakpoints in cold months (January to April, and November to December) is higher than in warm months (May to September) in every year. Previous documents and reports have also mentioned that the LST measurement instruments used for in situ observation systems have been gradually changed from manual to automatic ones since 2000 (Liu et al., 2008; Xu et al., 2019). Furthermore, it is well known that urbanization has developed rapidly during recent decades in China. The fact that some stations suffered from changes in the surrounding environment may also induce abrupt changes in the LST records, which is another reason for the increase in the number of breakpoints (Yan et al., 2010). Figure5. The number of effective breakpoints for the monthly LST records at the effective stations during 1960?2017; (a) the spatial distribution at all stations and (b) the accumulation in each month and each year across all stations.
2 3.3. Frequency distribution of adjustments in MASH -->
3.3. Frequency distribution of adjustments in MASH
To explore the LST adjustments identified in the MASH procedure, we count the number of effective breakpoints at all stations in each subregion and throughout the mainland of China. There are approximately 1.6 × 106 monthly records, of which 3.28 × 105 records (approximately 20% of the total records) show effective adjustments in MASH. In each subregion (Fig. 6), the majority of effective adjustments vary between 0.5oC and 1.5oC and between –0.5oC and –1.5oC (2.95 × 105 or 90% of all effective adjustments), within which two peaks are found around 0.5oC to 1.0oC and –0.5oC to –1.0oC. Except for the TB subregion, stations in other subregions show that the number of effective breakpoints with positive adjustments is greater than the number with negative ones. Moreover, minor adjustments are also counted in Fig. 7. We find that the minor adjustments account for 80% of the total adjustments in most subregions and in all of the mainland of China, which is consistent with the above results (effective adjustments records account for approximately 20% of the total records). Obviously, the percentage of minor adjustments in the SE subregion between July and October is low (less than 60%, red line with an inverted triangle in Fig. 7). This indicates that the percentage of effective adjustments in SE subregion is relatively large (over 40%). Except for the SE subregion, the YZ (NE) subregion in the cold season shows the highest (lowest) percentage of minor adjustments, above 90% (below 80%). Approximately 80% of the total records in the HHH subregion have experienced minor adjustments. Considering the large variability of the daily data, it is difficult to directly homogenize the daily time series. Therefore, MASH identifies the inhomogeneities from the monthly time series and applies the result to estimate the inhomogeneities of daily time series through smooth interpolation. We also plotted the frequency distribution of daily adjusted records (figures not shown) and it indeed exhibits similar characteristics with the monthly results. Figure6. Frequency distribution for the effective breakpoints of LST in the nine subregions and for the whole of the Chinese mainland. Biases at these breakpoints are adjusted with MASH.
Figure7. Percentage of records with adjusted LST biases between –0.5oC and 0.5oC in different months over the nine subregions and the whole of the Chinese mainland.