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Compared with the WRF_ERA5, the WRF_GCM significantly overestimated (underestimated) precipitation and SAT over the western North Pacific to the south (north) of 20°N (Figs. 3a, c). The error of SST in the large-scale forcing dataset shows a similar spatial pattern as that in the WRF_GCM, which indicates that the errors in precipitation and SAT possibly result from the SST bias over the western North Pacific (figure not shown). A warmer SST leads to higher SAT and more precipitation and vice versa. In contrast, the WRF_GCM significantly underestimated the precipitation, while overestimating the SAT over the Indian and Indochina Peninsula compared with the WRF_ERA5 (Figs. 3a, c). Notably, there is a consistency in the spatial patterns of overestimated SAT and underestimated precipitation over the land area. The decrease in precipitation is accompanied by increased downward solar radiation and a reduction in evapotranspiration from the land surface, which in turn leads to a higher SAT. The errors in downscaled precipitation and SAT are related to the errors in SST and upper-air variables, which will be further addressed in the next section. On the other hand, for the WRF_GCMbc, the errors in precipitation and SAT were significantly minimized for the entire domain (Fig. 3).
Figure 3. Mean errors of the precipitation (mm d–1) and surface air temperature (°C) in summer during the period 1982–2014. The shaded areas indicate regions where the error exceeds a significance level of 0.05.
In addition to the precipitation and SAT, other surface meteorological variables were also evaluated (Table 1). In comparison to the WRF_GCM, the WRF_GCMbc exhibited much smaller RMSEs in terms of the climatological means of the 2-m specific humidity, snow depth, sensible heat flux, latent heat flux, planetary boundary layer height, and 10-m wind speed. Generally, the RMSEs of the surface variables were reduced by 50%–80%. This improvement was more significant for summer than winter, especially for SAT, snow depth, sensible heat, latent heat, planetary boundary layer height, and 10-m wind speed. For example, the RMSE of SAT is reduced from 0.74°C in the WRF_GCM to 0.19°C in the WRF_GCMbc in summer. In contrast, the RMSE of SAT is reduced from 0.86°C in the WRF_GCM to 0.41°C in the WRF_GCMbc in winter. The errors in SAT primarily occur over mid-high latitudes and the Tibetan Plateau in winter, which is likely related to errors in the snow simulation (Meng et al., 2018).
SAT
(°C)SH2
(g kg–1)Precip
(mm d–1)Snowh
(mm)SHF
(W s–2)LHF
(W s–2)PBLH
(m)Wind10
(m s–1)(a) Climatological mean (WRF_GCM/WRF_GCMbc) Spring 0.87/0.18 0.69/0.13 3.15/0.95 4.46/1.62 6.07/2.23 15.34/5.25 42.49/16.99 0.42/0.14 Summer 0.74/0.19 0.69/0.13 3.37/1.05 2.61/0.70 6.77/1.63 21.94/4.53 53.11/14.65 0.69/0.16 Autumn 0.59/0.17 0.59/0.12 3.25/1.05 2.74/0.95 5.48/2.60 16.99/5.77 40.72/15.64 0.62/0.15 Winter 0.86/0.41 0.74/0.11 3.30/0.52 3.78/1.72 10.2/6.91 20.27/6.58 46.84/23.50 0.50/0.16 (b) Interannual-to-interdecadal standard deviation (WRF_GCM/WRF_GCMbc) Spring 0.34/0.23 0.26/0.11 1.79/1.00 1.76/0.86 3.77/1.96 6.90/3.52 22.36/12.93 0.19/0.08 Summer 0.29/0.13 0.27/0.09 1.95/0.93 1.25/0.54 3.20/1.20 7.01/3.82 20.02/11.12 0.21/0.11 Autumn 0.28/0.11 0.30/0.10 2.06/1.04 1.24/0.72 3.37/2.03 8.32/3.21 20.09/10.44 0.16/0.09 Winter 0.30/0.19 0.17/0.07 1.53/0.68 1.32/0.91 3.38/1.69 6.57/3.03 15.51/10.07 0.15/0.08 (c) Day-to-day variability (WRF_GCM/WRF_GCMbc) Spring 0.13/0.05 0.08/0.04 0.22/0.10 1.39/0.52 1.61/0.66 3.58/1.71 9.28/4.47 0.11/0.07 Summer 0.08/0.05 0.09/0.03 0.27/0.11 0.08/0.03 1.18/0.44 4.50/1.41 8.59/3.94 0.18/0.06 Autumn 0.15/0.05 0.09/0.04 0.28/0.10 0.10/0.05 1.83/0.81 4.92/1.71 10.25/4.41 0.20/0.07 Winter 0.20/0.09 0.09/0.03 0.26/0.06 1.41/0.62 2.71/1.52 4.36/1.67 11.94/5.58 0.13/0.06 SAT: surface air temperature, SH2: 2-m specific humidity, Precip: precipitation, Snowh: snow depth, SHF: sensible heat flux, LHF: latent heat flux, PBLH: planetary boundary layer height, Wind10: 10-m wind speed. Table 1. RMSEs for the climatological mean, interannual-to-interdecadal, and day-to-day variabilities of various variables in different seasons calculated within the verification region illustrated in Fig. 2.
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We also computed the RMSEs of downscaled upper-air temperature, geopotential height, vector wind, and relative humidity in summer (Fig. S4 in the ESM). The WRF_GCM showed that the largest RMSEs for the air temperature, geopotential height, and vector wind occur in the upper troposphere, while those for relative humidity occur in the mid-troposphere. Compared with the WRF_GCM, the WRF_GCMbc showed much smaller RMSEs of upper-air variables in all vertical levels in summer (Fig. S4 in the ESM). Generally, the RMSEs of downscaled upper-air variables were reduced by approximately 70%–90% due to the GCM bias corrections. Similarly, the WRF_GCMbc also exhibited significant improvement in simulating upper-air variables in other seasons (figure not shown).
Figure 4 illustrates the spatial pattern of climatological mean errors in 850-hPa geopotential height, vector wind, and relative humidity in summer. Compared with the WRF_ERA5, the WRF_GCM significantly underestimated the geopotential height over the western North Pacific between 5°N and 30°N, while overestimating it across the Asian continent and western North Pacific to the north of 30°N. In association with the geopotential height errors, the 850-hPa vector wind showed a significant cyclonic error in the western North Pacific between 5°N and 30°N and an anticyclonic error around the Tibetan Plateau (Fig. 4a). The anticyclonic error in 850-hPa vector wind and the negative error in relative humidity corresponded to dry and warm errors over India and the Bay of Bengal. Similarly, the cyclonic error and the positive error in relative humidity were associated with an overestimation of precipitation over the western North Pacific between 5°N and 20°N in the WRF_GCM relative to the WRF_ERA5 (Figs. 3a, c and 4a, c). We also noted a spatial consistency in the patterns of errors for both the 850-hPa geopotential height and vector wind between the WRF_GCM and MPI-ESM1-2-HR (figure not shown). This indicates that the errors in the downscaled 850-hPa circulations are largely inherited from the large-scale forcing data. In terms of the simulation of 850-hPa relative humidity, the WRF_GCM also exhibited significant errors relative to the WRF_ERA5, with an overestimation over the western North Pacific and equatorial Indian Ocean and an underestimation over India and the Bay of Bengal (Fig. 4c). Overall, the downscaled circulation, relative humidity, precipitation, and SAT improved significantly due to the GCM bias corrections (Figs. 3 and 4).
Figure 4. Mean errors of 850-hPa geopotential height (gpm), vector wind (m s–1), and relative humidity (g kg–1) in summer (June–July–August) for the period 1982–2014. Shaded areas represent the errors reaching the 0.05 significance level. The red, blue, and black arrows indicate that the zonal wind, meridional wind, or both of them have reached a significance level of 0.05, respectively.
Notably, the GCM bias correction leads to a more significant improvement in dynamical downscaling simulations compared with that presented in Xu and Yang (2012), especially in the lower troposphere. In the previous study, the dynamical downscaling simulations were forced by observed SST data, and the GCM bias corrections were only applied to the upper-air variables (Xu and Yang, 2012). In contrast, the upper-air variables and SST biases were simultaneously corrected in this study. The additional bias corrections to SST lead to a greater improvement in the dynamical downscaling simulations, especially for the lower tropospheric variables.
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The onset of the SCS summer monsoon generally occurs around mid-May, which signifies the beginning of the East Asian summer monsoon (Wang et al., 2004). Following Wang et al. (2004), the South China Sea (SCS) monsoon index, uSCS, is defined as the 850-hPa zonal wind averaged over the central SCS (5°–15°N, 110°–120°E). The climatological mean uSCS shows an abrupt seasonal transition from easterly to westerly around mid-May associated with the onset of SCS summer monsoon. The dynamical downscaling simulations were able to reasonably capture the annual cycle of uSCS (Fig. S5 in the ESM). The climatological mean uSCS showed a transition from easterly to westerly around early May in the WRF_ERA5 and WRF_GCMbc. In contrast, the transition occurred in mid-May in the WRF_GCM. The transition from westerly to easterly winds became evident in mid-October in all three WRF simulations. The uSCS derived from the large-scale forcing data (i.e., the ERA5 reanalysis, raw GCM, and the bias-corrected CMIP6 data) showed similar annual cycles as those in the WRF simulations (figure not shown). The only exception was noted for the transition date from easterly to westerly, which occurred almost 10 days later than that in the WRF simulations (Fig. S5 in the ESM). This indicates that the downscaled annual cycle of the SCS monsoon circulation is strongly affected by the large-scale forcing data. However, the WRF simulations tended to generate an earlier onset of westerly flow by approximately 10 days compared to the corresponding large-scale forcing data, which can be attributed to the WRF model bias.
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In addition to climatological means, temporal variability is also of great importance in the future projection of regional climate and its impacts. Here, the interannual-to-interdecadal variability is measured by the standard deviation of a seasonal mean scalar or vector variable over the period 1982–2014 (Eqs. 2 and 3). Compared with the WRF_ERA5, the WRF_GCM significantly underestimated the interannual-to-interdecadal variability of precipitation over India, the Bay of Bengal, and the South China Sea. In contrast, it overestimated the precipitation variability over the western North Pacific to the south of 20°N (Figs. S6a, b in the ESM). Notably, the spatial patterns of the errors in precipitation variability were consistent with those found for the climatological mean. The errors in precipitation variability were significantly reduced in the WRF_GCMbc. For example, the RMSE of summer precipitation variability was reduced from 1.95 mm d–1 in the WRF_GCM to 0.93 mm d–1 in the WRF_GCMbc (Table 1). Compared with the WRF_ERA5, the WRF_GCM underestimated the interannual-to-interdecadal variance of summer SAT in northwestern India and eastern China while overestimating it over the Bay of Bengal, Indochina Peninsula, and the western North Pacific to the south of 30°N. The errors in the interannual-to-interdecadal variance of downscaled SAT were also greatly reduced in the WRF_GCMbc due to the GCM bias correction (Figs. S6c, d in the ESM).
Similar to precipitation and SAT, other surface variables also exhibited significant improvements in their interannual-to-interdecadal variability in the WRF_GCMbc relative to the WRF_GCM with a reduction of almost 30%–60% in RMSEs (Table 1). Among these surface variables, 2-m specific humidity showed the most pronounced improvement with a decrease in the RMSE by roughly 60%. Overall, the improvement in the downscaled interannual-to-interdecadal variability was relatively small compared with that of the climatological means.
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The GCM bias correction significantly improved the interannual-to-interdecadal variability of upper air temperature, geopotential height, vector wind, and relative humidity at all vertical levels in summer (Fig. S7 in the ESM) as well as in other seasons (figure not shown). The RMSEs in the interannual-to-interdecadal variability were reduced by 20%–70%. Note that this improvement was smaller than that in climatological means (Figs. S4 and S7 in the ESM). This indicates that it is more challenging to improve downscaled temporal variability than the climatological means by correcting the GCM biases.
Compared with the WRF_ERA5, the WRF_GCM significantly underestimated the interannual-to-interdecadal variability of the 850-hPa geopotential height over the Eastern China-East China Sea and conversely overestimated it over the Maritime Continent and western North Pacific to the east of 140°E (Fig. S8a in the ESM). This suggests that the western North Pacific subtropical high (WNPSH) exhibited a weaker interannual-to-interdecadal variability over East Asia to the south of 40°N in the WRF_GCM than in the WRF_ERA5. In this region, the 850-hPa vector wind also showed a weaker interannual-to-interdecadal variability over eastern China and the South China Sea, which may be linked to the reduced summer precipitation variability in the WRF_GCM (Figs. S6a and S8c in the ESM). Conversely, the WRF_GCM overestimated the vector wind variability over the western North Pacific to the south of 20°N where it also showed an overestimation of precipitation variability relative to the WRF_ERA5. It appears that the variability of the 850-hPa vector wind can partially account for the precipitation variability. In the WRF_GCMbc, the errors in the interannual-to-interdecadal variability of the geopotential height and vector wind were largely removed due to the GCM bias corrections. Consequently, the variability of downscaled precipitation was improved in the WRF_GCMbc.
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The onset of SCS summer monsoon shows considerable year-to-year variability (Wu and Wang, 2001; Jiang and Zhu, 2021). To examine the temporal variability of the SCS summer monsoon, we defined the onset date of the SCS summer monsoon as the first day after 25 April, where the 5-day running mean of uSCS is greater than 1 m·s-1 and persists for at least 15 days. The variance of SCS summer monsoon onset date was 11.9, 10.6, and 12.6 days in the WRF_ERA5, WRF_GCM, and WRF_GCMbc, respectively (Fig. S9 in the ESM). Clearly, compared with the WRF_GCM, the WRF_GCMbc generated an SCS summer monsoon variability closer to that in the WRF_ERA5. Moreover, both the WRF_GCMbc and WRF_ERA5 showed a clear decline in the onset date of SCS summer monsoon over the period 1982–2014, which was not evident in the WRF_GCM. As discussed in section 2.2, the MME generally shows a more consistent non-linear trend with the ERA5, relative to individual CMIP6 models, which likely helps improve the long-term trend of onset date of the downscaled SCS summer monsoon.
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It is known that the leading mode of the Empirical Orthogonal Function (EOF) for the observed summer precipitation shows a dry-wet-dry pattern over the North China-Yangtze River Basin-South China at interannual to interdecadal time scales (Ding et al., 2008). Previous studies suggested that both internal climate variability and external forcing contribute to the precipitation anomalous mode (Yang et al., 2017; Huang et al., 2023). The WRF_ERA5 can reasonably reproduce the tri-pole pattern (–, +, –) of the observed summer precipitation anomaly, characterized by a positive precipitation anomaly over the Yangtze River basin and a negative precipitation anomaly over North China and South China (Fig. 5a). However, the WRF_GCM showed a monopole pattern over eastern China, instead (Fig. 5b). This indicates that summer precipitation varies homogeneously over eastern China in the WRF_GCM. In contrast, the WRF_GCMbc successfully reproduced the tri-pole pattern of summer precipitation anomaly due to the GCM bias corrections (Fig. 5c). In addition to the first EOF mode, the second and third EOF modes in the WRF_GCMbc were also more consistent with those in the WRF_ERA5 relative to the WRF_GCM (Table S1 in the ESM). The first three EOF modes accounted for 52.3%, 43.1%, and 51.4% of the total variance in the WRF_ERA5, WRF_GCM, and WRF_GCMbc, respectively. Note that the WRF_GCMbc well captured the declining trend of the time series of the leading EOF, which is likely due to the improved long-term trend in the MME relative to individual CMIP6 models (Figs. 5a, c and Fig. S1 in the ESM).
Figure 5. Leading EOF mode, PC time series of summer precipitation anomaly (mm d–1, bars), and its trend (thick black line) derived from the WRF_ERA5, ERA_GCM, and WRF_GCMbc, respectively. The variance explained is shown on the top of each panel.
As discussed in section 3.3, the interannual variability of precipitation is related to that of the atmospheric circulation. Therefore, we computed the difference of the 850-hPa geopotential height, vector wind, and moisture between the positive- and negative-phase years of the leading EOF time series. The positive (negative) phase years were defined as the time series of an EOF greater (smaller) than a 0.5 (–0.5) standard deviation. In the positive-phase years, the 850-hPa geopotential height showed a positive (negative) anomaly to the south (north) of 30°N, indicating a southward shift of the WNPSH in the WRF_ERA5 (Fig. 6a). Correspondingly, the 850-hPa circulation revealed an anticyclonic (cyclonic) anomaly to the south (north) of 30°N in the positive-phase years and corresponded to a dry anomaly over South China (Figs. 5a, 6a). The Yangtze River basin was dominated by a southwesterly anomaly, which may bring abundant moisture and a wet anomaly. The southward shift of WNPSH hiders the northward transfer of moisture and results in a dry anomaly over North China (Fig. 6a). The spatial patterns of the 850-hPa geopotential height and vector wind anomalies in the WRF_GCMbc were consistent with those in the WRF_ERA5. Consequently, the WRF_GCMbc well captured the leading EOF of summer precipitation anomaly. In contrast, the WRF_GCM generated a positive 850-hPa geopotential height anomaly over East Asia between 20°N and 40°N in the positive-phase years relative to the negative-phase years (Fig. 6b). In turn, the enhanced WNPSH causes a dry anomaly over eastern China and vice versa.
Figure 6. Differences in the 850-hPa geopotential height (m2 s–2), vector wind (m s–1), and moisture (g kg–1) between the positive and negative phase years. A positive (negative) year is defined by the time series of the first EOF (Fig. 5) greater (smaller) than its 0.5 (–0.5) standard deviation. The contour and its color represent geopotential height and specific humidity, respectively.
Figure 7 further illustrates the contours of 1500 geopotential meters (gpm) and 1450 gpm of the summer WNPSH in the WRF_ERA5, WRF_GCM, and WRF_GCMbc throughout 1982–2014. The 1500-gpm contour can roughly illustrate the location of the WNPSH. Based on the geostrophic balance between the geopotential height and wind, wind generally flows along the isobars. Thus, the 1450-gpm contour can roughly represent the 850-hPa prevailing wind direction over eastern China. In the WRF_ERA5, the WNPSH extended southwestward in the positive-phase years, leading to a positive (negative) geopotential height anomaly to the south (north) of 30°N (Figs. 6a and 7a). The prevailing wind flows from the Indo-China peninsula to the East China Sea as indicated by the 1450-gpm contour in the positive-phase years, which brings more precipitation to the Yangtze River basin and less precipitation to South China and North China (Figs. 5a, 6a, and the red lines in Fig. 7d). In the negative-phase years, the WNPSH extended northward and the 1450-gpm contour showed a south-north orientation, which can bring more moisture and precipitation to North China (blue lines in Figs. 7a, d). However, the WRF_GCM demonstrated less skill in capturing the location of the WNPSH ridge, which was characterized by a roughly 5-degree northward migration relative to that in the WRF_ERA5 (Figs. 7a, b). The 1450-gpm contour extended westward in the positive-phase years relative to the negative-phase years over eastern China between 20°N and 40°N, inducing a monopole pattern of summer precipitation anomaly (Figs. 5b and 7e). Notably, the error in the location of the WNSPH ridge was greatly reduced in the WRF_GCMbc due to the GCM bias corrections (Figs. 7a–c). Moreover, the 1450-gpm contours revealed a very similar spatial pattern between 20°N and 40°N as that in the WRF_ERA5, i.e., a southwest-northeast orientation in the positive-phase years and a south-north orientation in the negative phase years (Figs. 7d, f). This spatial pattern of geopotential height is crucial for generating the leading EOF pattern of the observed summer precipitation anomaly over eastern China.
Figure 7. The 1500-gpm and 1450-gpm contours of geopotential heights in the (a, d) WRF_ERA5, (b, e) WRF_GCM, and (c, f) WRF_GCMbc for positive-phase (red line), negative-phase (blue line), and normal years (grey line) from 1982–2014. The thick red and blue contours represent the geopotential height averaged over the positive-phase and negative-phase years, respectively. The positive (negative) years are the same as in Fig. 6.
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To evaluate the downscaled intraseasonal oscillation (ISO), we calculated the variance of the 20–100-day filtered precipitation averaged in the summer and winter half of the year (Fig. 8). Compared with the WRF_ERA5, the WRF_GCM significantly underestimated the ISO strength over South and Southeast Asia, while overestimating it over the western North Pacific (5°–20°N, 140°–165°E) in the summer half year (Fig. 8a). In the WRF_GCMbc, the mean error of the ISO strength was greatly reduced compared to the WRF_GCM, suggesting that the GCM bias correction can significantly improve the downscaled ISO strength over the Asia-western North Pacific domain (Figs. 8a, b). Moreover, the variance of 20–100-day filtered 850-hPa zonal wind showed similar errors to those of precipitation either in the WRF_GCM or its large-scale forcing data. These errors were greatly reduced after GCM bias correction (figures not shown). This indicates that the RCM simulation driven by the bias-corrected CMIP6 data can well capture the ISO intensity of downscaled precipitation. Similar to the summer half-year, GCM bias correction can also significantly improve the downscaled ISO in the winter half-year (Figs. 8c, d).
Figure 8. Mean errors of the standard deviation of the 20–100-day filtered intraseasonal precipitation (mm d–1) for the summer (May–October) and winter (November–April) half-year averaged over the period 1982–2014. The hatched area indicates that the difference reached the significance level of 0.05.
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The day-to-day (DTD) temperature variability, defined as the mean absolute difference of the surface air temperature between two adjacent days, is one of the important factors that likely affect human health (Liu et al., 2020; Xu et al., 2020). Compared with the WRF_ERA5, the WRF_GCM significantly overestimated the DTD temperature variability by 0.1°C–0.4°C across the Asian continent, while underestimating it by 0.1°C–0.3°C over the western North Pacific between 20°N and 40°N (Fig. 9a). These errors in the downscaled DTD temperature variability were greatly reduced in the WRF_GCMbc due to the GCM bias correction (Figs. 9a, b).
Figure 9. Mean error of day-to-day variability of 2-m air temperature (units: °C), 850-hPa meridional wind and climatological mean meridional temperature gradient [units: °C (100 km)–1] at 850 hPa in winter (December–January–February) during the period 1982–2014. The mean errors in (c) and (d) were calculated with the absolute value of temperature gradient derived from the WRF_GCM (WRF_GCMbc) and WRF_ERA5. The hatched area indicates that the error reached a significance level of 0.05.
It is known that temperature advection is one of the key factors that affect DTD temperature variability (e.g., Xu et al., 2020). To identify the source of error in DTD temperature variability, we calculated the climatological mean meridional temperature gradient and DTD variability of the 850-hPa meridional wind (Figs. 9c–f). Compared with the WRF_ERA5, the WRF_GCM overestimated the temperature gradient over the Asian continent to the north of 35°N, which is favorable for increasing the temperature advection and DTD temperature variability there. Similarly, the reduced temperature gradient over the western North Pacific corresponded to a decrease in DTD temperature variability between 20°N and 40°N (Figs. 9a, c). However, the increase in DTD temperature variability over southern China and northern India may be attributed to enhanced DTD variability of the 850-hPa meridional wind rather than the temperature gradient (Figs. 9a, c, e). The GCM bias correction significantly reduced the errors in the downscaled 850-hPa temperature gradient and the daily 850-hPa meridional wind variability, leading to an improvement in DTD temperature variability (Fig. 9).
SAT (°C) |
SH2 (g kg–1) |
Precip (mm d–1) |
Snowh (mm) |
SHF (W s–2) |
LHF (W s–2) |
PBLH (m) |
Wind10 (m s–1) |
|
(a) Climatological mean (WRF_GCM/WRF_GCMbc) | ||||||||
Spring | 0.87/0.18 | 0.69/0.13 | 3.15/0.95 | 4.46/1.62 | 6.07/2.23 | 15.34/5.25 | 42.49/16.99 | 0.42/0.14 |
Summer | 0.74/0.19 | 0.69/0.13 | 3.37/1.05 | 2.61/0.70 | 6.77/1.63 | 21.94/4.53 | 53.11/14.65 | 0.69/0.16 |
Autumn | 0.59/0.17 | 0.59/0.12 | 3.25/1.05 | 2.74/0.95 | 5.48/2.60 | 16.99/5.77 | 40.72/15.64 | 0.62/0.15 |
Winter | 0.86/0.41 | 0.74/0.11 | 3.30/0.52 | 3.78/1.72 | 10.2/6.91 | 20.27/6.58 | 46.84/23.50 | 0.50/0.16 |
(b) Interannual-to-interdecadal standard deviation (WRF_GCM/WRF_GCMbc) | ||||||||
Spring | 0.34/0.23 | 0.26/0.11 | 1.79/1.00 | 1.76/0.86 | 3.77/1.96 | 6.90/3.52 | 22.36/12.93 | 0.19/0.08 |
Summer | 0.29/0.13 | 0.27/0.09 | 1.95/0.93 | 1.25/0.54 | 3.20/1.20 | 7.01/3.82 | 20.02/11.12 | 0.21/0.11 |
Autumn | 0.28/0.11 | 0.30/0.10 | 2.06/1.04 | 1.24/0.72 | 3.37/2.03 | 8.32/3.21 | 20.09/10.44 | 0.16/0.09 |
Winter | 0.30/0.19 | 0.17/0.07 | 1.53/0.68 | 1.32/0.91 | 3.38/1.69 | 6.57/3.03 | 15.51/10.07 | 0.15/0.08 |
(c) Day-to-day variability (WRF_GCM/WRF_GCMbc) | ||||||||
Spring | 0.13/0.05 | 0.08/0.04 | 0.22/0.10 | 1.39/0.52 | 1.61/0.66 | 3.58/1.71 | 9.28/4.47 | 0.11/0.07 |
Summer | 0.08/0.05 | 0.09/0.03 | 0.27/0.11 | 0.08/0.03 | 1.18/0.44 | 4.50/1.41 | 8.59/3.94 | 0.18/0.06 |
Autumn | 0.15/0.05 | 0.09/0.04 | 0.28/0.10 | 0.10/0.05 | 1.83/0.81 | 4.92/1.71 | 10.25/4.41 | 0.20/0.07 |
Winter | 0.20/0.09 | 0.09/0.03 | 0.26/0.06 | 1.41/0.62 | 2.71/1.52 | 4.36/1.67 | 11.94/5.58 | 0.13/0.06 |
SAT: surface air temperature, SH2: 2-m specific humidity, Precip: precipitation, Snowh: snow depth, SHF: sensible heat flux, LHF: latent heat flux, PBLH: planetary boundary layer height, Wind10: 10-m wind speed. |