Solar radiation modification (SRM) is a potential strategy to rapidly mitigate global warming by reflecting more sunlight into space. However, its impact on tropical hydrological cycles remains underexplored. This study investigates the potential effects of SRM on streamflow in the Kelantan River Basin (KRB) by incorporating climate projections from the Geoengineering Model Intercomparison Project Phase 6 (GeoMIP6) into the Soil and Water Assessment Tool plus (SWAT+) model. Results indicate that UKESM1-0-LL and MPI-ESM1-2-LR exhibit higher uncertainty in representing KRB's climate compared to CNRM-ESM2-1 and IPSL-CM6A-LR. Under SSP5-8.5, maximum and minimum temperatures are projected to increase by up to 3.52 °C by the late 21st century, while SRM scenarios may limit warming to 1.72-2.33 °C, similar to 1.96-2.22 °C under SSP2-4.5. The multi-model ensemble mean projected an inverse V-shaped trend in annual precipitation, with a peak in the mid-21st century before declining, except for G6sulfur, which exhibits a steady decrease. Increases in monthly precipitation from November to January during the 2045-2064 period under all evaluated scenarios may intensify flooding in the KRB. Meanwhile, decreases in streamflow during dry months are projected for the periods 2045-2064 and 2065-2085 under G6sulfur, particularly in the middle and upper basins.

  • Integrating GeoMIP6 data into SWAT+ to examine SRM effects in the global south.

  • UKESM1-0-LL shows higher uncertainties than other models.

  • G6solar and G6sulfur could effectively cool temperature increases under SSP5-8.5.

  • More severe floods might occur in the 2045–2064 period.

  • G6sulfur could potentially exacerbate the water shortage problem in the basin.

Since the pre-industrial era, human activities have increased greenhouse gas concentrations, which are the primary drivers of global warming (Masson-Delmotte et al. 2021). A direct consequence of global warming is the rise in atmospheric temperatures, leading to enhanced evaporation and an increased capacity of the atmosphere to hold water vapor. The intensification of the hydrological cycle exacerbates heavy precipitation and flooding but may also contribute to prolonged drought periods in terrestrial regions (Masson-Delmotte et al. 2021). In other words, wet areas are expected to become even wetter in the future, while dry regions may become drier (Held & Soden 2006).

With insufficient efforts to reduce CO2 emissions, solar radiation modification (SRM) has emerged as one of the most discussed strategies for preventing global temperature from rising more than 1.5 °C above the pre-industrial level. SRM aims to rapidly cool the Earth by reducing incoming shortwave radiation to offset the warming effects (Crutzen 2006; Masson-Delmotte et al. 2021). Hydro-climatic SRM studies primarily focus on extreme temperatures, extreme precipitation (Jones et al. 2013), throughflow (Shen et al. 2023), streamflow (Tan et al. 2023b), evaporation (MacMartin et al. 2022), and snowmelt (Ridley & Blockley 2018). Among these hydrological components, studying streamflow provides valuable insights into water availability and related disasters such as floods and droughts. Compared to Representative Concentration Pathways (RCP) 4.5, the GeoMIP G4 scenario results in increased streamflow in western Eurasia and North America, alongside reduced streamflow in their eastern part (Wei et al. 2018). Under the G1 or 4 × CO2 scenario, Tilmes et al. (2013) reported a global precipitation increase of approximately 6.9%, accompanied by notable zonal and regional differences. For instance, precipitation increased by 10% over Asia and decreased by 7% in the North American summer monsoon. In Africa, the likelihood of dry conditions increased, while the probability of wet conditions declined during the installation and termination stages of Stratospheric aerosol injection (SAI) (Obahoundje et al. 2023).

In recent years, scholars have raised concerns about the validity of simulating SRM scenarios (Visioni et al. 2023). The Geoengineering Model Intercomparison Project (GeoMIP), a sub-project of CMIP6, provides a standardized framework for SRM modeling experiments, enabling more robust comparisons of model responses and uncertainties. In the sixth phase of GeoMIP (GeoMIP6), the G6solar and G6sulfur experiments were proposed to transition radiative forcing from the high-emission scenario (Shared Socioeconomic Pathway 5-8.5; SSP5-8.5) (Meinshausen et al. 2020) to the intermediate-emission scenario (SSP2-4.5) by reducing the solar constant or injecting SO2 into the stratosphere. Based on the GeoMIP6 guideline, the mean global 2 m air temperature under the G6solar or G6sulfur scenarios must be within 0.2 K of the corresponding decade for each model's SSP2-4.5 simulation from 2021 to 2100 (Kravitz et al. 2021). Visioni et al. (2021) reported that the global mean precipitation response during the 2081–2100 period is projected to vary from −3.79 ± 0.76 % for G6sulfur and −2.07% ± 0.40% for G6solar compared to SSP2-4.5. Similar GeoMIP6 studies have explored regional scales, including China (Wang et al. 2023), East Asia (Liang & Haywood 2023), and Indonesia (Shen et al. 2023). However, there is a notable lack of research on SRM impacts across Southeast Asia, particularly at localized and river basin scales.

The Kelantan River Basin (KRB) in Malaysia experiences frequent floods almost every year during the first phase of the northeast monsoon season, which spans from November to mid-January (Tan et al. 2021). Additionally, the KRB faces dry conditions during the second phase of the northeast monsoon and the first inter-monsoon, typically from February to May. These dry conditions reduce water availability and affect freshwater supply, as the basin lacks reservoirs to store water for the dry seasons. Monthly precipitation and streamflow in the KRB are projected to become more frequent and intense, according to simulations from 36 downscaled climate projections from CORDEX-SEA (Tan et al. 2017a, 2020). Tan et al. (2023b) were the first to investigate the impact of SRM in the KRB using Stratospheric Aerosol Geoengineering Large Ensemble (GLENS) members. They found that SRM could reduce precipitation during flooding months compared to RCP8.5, but it would also decrease precipitation during dry months. However, the GLENS model may not adequately address uncertainties from different climate models. Furthermore, it relies on simplified assumptions about SRM and primarily focuses on temperature control, potentially overlooking other SRM strategies such as G6solar and G6sulfur.

Previous research has demonstrated that SRM could effectively lower mean temperature; however, its impact on tropical precipitation and streamflow, which exhibit greater variability than other variables, remains unclear. Therefore, this study aims to develop a comprehensive and up-to-date hydro-climatic assessment framework for evaluating the impact of SRM on tropical hydro-climatic changes. Three specific objectives of this study are (1) to apply bias correctly to GeoMIP6 models, including CNRM-ESM2-1, IPSL-CM6A-LR, MPI-ESM1-2-LR, and UKESM1-0-LL; (2) to calibrate and validate the Soil and Water Assessment Tool plus (SWAT+) model for simulating streamflow in the KRB; and (3) to assess potential hydro-climatic changes in the KRB for the near-term (2025–2044), mid-term (2045–2064), and end-term (2065–2084) of the 21st century compared to the baseline period (1985–2004) under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios. This study is among the first to apply SRM scenarios from GeoMIP6 at the river basin scale in Southeast Asia, providing new insights into the potential impacts of SRM on local climate dynamics and the hydrological cycle. Understanding these localized effects is crucial for developing countries that are particularly vulnerable to climate change, as it allows them to assess how SRM might affect their specific water resource systems, thereby supporting decision-making and policy development. Additionally, the findings can serve as a reference for the GeoMIP community in formulating more realistic SRM strategies for the upcoming GeoMIP7 scenarios.

The KRB is the second-largest basin in Peninsular Malaysia (Figure 1), located between latitudes 4° and 6° and longitudes 101 and 102°, covering an area of 12,685 km2 (Tan et al. 2023a). The mean annual precipitation is 2,700 mm/year, with temperatures ranging from 23 to 34.8 °C. Influenced by the monsoons, the heaviest precipitation normally occurs from November to mid-January. The elevation within the basin ranges from −26 to 2,173 m above mean sea level. Forests cover approximately 70% of the total area, with oil palm and rubber as the primary crops. Agricultural land is concentrated in the central, downstream, and southeastern parts of the basin. The basin is bordered by mountains to the east, west, and south (Suhana et al. 2023).
Figure 1

Topography and distribution of stations in the KRBasin, Malaysia.

Figure 1

Topography and distribution of stations in the KRBasin, Malaysia.

Close modal

GEOMIP6

The SWAT model, widely used in Southeast Asia (Tan et al. 2019), requires long-term, continuous daily data for precipitation, maximum temperature, and minimum temperature. Among the GeoMIP6 models, only CESM2-WACCM, IPSL-CM6A-LR, UKESM1-0-LL, MPI-ESM1.2-LR, and CNRM-ESM2-1 simulate these daily meteorological variables. However, the CESM2-WACCM model does not provide temperature data for historical periods (Visioni et al. 2023; Tan et al. 2024), preventing the use of observed data for bias correction. Therefore, this study utilizes the other four GeoMIP models listed in Table 1. The general findings are reported based on the ensemble mean data from these four models.

Table 1

Four GeoMIP models used in this study

ModelsInstitutionResolutionReference
CNRM-ESM2-1 Centre National de Recherches Météorologiques (CNRM), France H: 1.4° × 1.4°; V: 40 Séférian et al. (2019)  
MPI-ESM1.2-LR Max Planck Institute for Meteorology (MPI-M), Germany H: 1.9° × 1.9°; V: 47 Müller et al. (2018)  
IPSL-CM6-LR Institut Pierre-Simon Laplace (IPSL), France H: 2.5° × 1.3°; V: 79 Madeleine et al. (2020)  
UKESM1-0-LL Met Office Hadley Centre,UK H: 1.9° × 1.3°; V: 85 Sellar et al. (2019)  
ModelsInstitutionResolutionReference
CNRM-ESM2-1 Centre National de Recherches Météorologiques (CNRM), France H: 1.4° × 1.4°; V: 40 Séférian et al. (2019)  
MPI-ESM1.2-LR Max Planck Institute for Meteorology (MPI-M), Germany H: 1.9° × 1.9°; V: 47 Müller et al. (2018)  
IPSL-CM6-LR Institut Pierre-Simon Laplace (IPSL), France H: 2.5° × 1.3°; V: 79 Madeleine et al. (2020)  
UKESM1-0-LL Met Office Hadley Centre,UK H: 1.9° × 1.3°; V: 85 Sellar et al. (2019)  

Note: H indicates horizontal resolution; V indicates vertical layers.

Kravitz et al. (2015) proposed G6solar and G6sulfur as part of the standard experiments in GeoMIP6. These experiments aim to reduce global mean temperatures from the high-emission SSP5-8.5 scenario to the moderate-emission SSP2-4.5 scenario. IPSL-CM6A-LR and UKESM1-0-LL are adjusted every 10 years, based on changes in the solar constant or specified increases in stratospheric SO2 or aerosol, to achieve a surface temperature reduction aligning with SSP2-4.5. In contrast, MPI-ESM1.2-LR and CNRM-ESM2-1 implemented these adjustments annually (Visioni et al. 2021, 2023).

Daily observed precipitation, maximum temperature and minimum temperature data from 23 meteorological stations, well distributed across the basin, as shown in Figure 1, were obtained from the Malaysian Meteorological Department (Tan et al. 2017b). The GeoMIP6 climate models were bias-corrected using the linear scaling (LSC) method before analyzing basin-scale climatic changes and incorporating them into the SWAT+ model for hydrological analysis. The LSC method was employed for its simplicity and efficiency (Lenderink et al. 2007). Bias correction of the GeoMIP6 models was performed using the Climate Model data for Hydrological Modeling (CMhyd) tool, developed by Rathjens et al. (2016). This tool is freely available at https://swat.tamu.edu.software/cmhyd/. The LSC formula for correcting precipitation and temperature is provided as follows:
(1)
(2)
where and represent the corrected GeoMIP6 daily precipitation data from 1985 to 2004 and 2021 to 2100, respectively, whereas and represent the raw GeoMIP6 and observed daily precipitation data from 1985 to 2004, respectively. The symbol d refers to daily data, and μ indicates the monthly mean.
(3)
(4)

Similarly, and represent the corrected GeoMIP6 daily temperature data from 1985 to 2004 and 2021 to 2100, respectively, whereas and represent the raw GeoMIP6 and observed daily temperature data from 1985 to 2004, respectively. Besides that, the climatological characteristics of the original and bias corrected data from the four GeoMIP6 datasets are evaluated against observations.

SWAT +

The SWAT model is one of the most widely used hydrologic models in basins worldwide for the past decades (Arnold et al. 1998). In this study. the SWAT+ model, an upgraded version of the SWAT model, was used. The SWAT is based on the hydrological response unit (HRU), which consists of areas with similar soil, slope, and land use features. In the SWAT, HRUs are defined within a sub-basin, while in SWAT + , HRUs are specified within a smaller unit called the landscape unit, which is a sub-unit that forms the sub-basin. The SWAT+ model retains the same fundamental methods for calculating physical processes but introduces significant changes in the structure and organization of the input code and files (Andaryani et al. 2021; Rathjens et al. 2022).

The soil type and land use maps were used to generate the HRUs. The digital elevation model (DEM) was used to generate river networks and the slope of the basin. Observed daily precipitation, maximum temperature, and minimum temperature data collected from 1985 to 2004 were used to run the model. Monthly streamflow data obtained from the Department of Irrigation and Drainage Malaysia were used to calibrate and validate the SWAT+ model for the same period, from January 1985 to December 2004. The SWAT+ toolbox was used for sensitivity analysis, model calibration, and verification. Based on the parameters employed in the calibration of the SWAT+ model by Tan et al. (2023b) and Yang et al. (2022), a total of 14 parameters were identified, as shown in Table 2. Among them, curve number condition II (CN2) and lateral flow coefficient (LATQ_CO) were identified as the most sensitive parameters for the KRB, which is consistent with the findings reported by Tan et al. (2023b). The fitted values indicate the optimal parameter values for accurately simulating streamflow in the KRB. This study utilized two popular statistical methods, Nash–Sutcliffe Efficiency (NSE) and coefficient of determination (R2), to assess the performance of the SWAT in simulating streamflow. The performance of the SWAT can be categorized as ‘very good’ if NSE > 0.8 and R2 > 0.85, ‘good’ if NSE > 0.7 and R2 > 0.75, ‘satisfactory’ if NSE > 0.5 and R2 > 0.6 (Tan et al. 2021). Similarly, the SWAT+ model was evaluated using these standards.

Table 2

SWAT+ parameters selected for sensitivity analysis and calibration

No.Parameter nameParameterMinimum valueMaximum valueCHG_TYPFitted value
Lateral soil flow coeff-linear adj to daily lateral flow LATQ_CO absval 0.94 
Initial SCS CN II value CN2 −20 20 pctchg −19.04 
Effective hydraulic conductivity in main channel alluvium CHK −0.01 500 absval 9.89 
Groundwater ‘revap’ coefficient REVAP_CO 0.02 0.2 absval 0.2 
Plant water uptake compensation factor EPCO absval 0.323 
Maximum canopy storage CANMX 20 absval 19.89 
Percolation coefficient bottom soil layer due to an impermeable layer or high water table PERCO 0.8 absval 0.97 
Available water capacity AWC −20 20 pctchg −1.62 
Average slope steepness in HRU SLOP 0.01 0.9 absval 0.6 
10 USLE equation support practice (P) factor USLE_P absval 0.32 
11 Threshold depth of water in the shallow aquifer for ‘revap’ to occur REVAP_MIN 50 absval 30.42 
12 Lateral flow travel time LAT_TTIME 0.5 180 absval 110.39 
13 Lag factor for gw recession curve ALPHA absval 0.45 
14 Threshold depth of water in the shallow aquifer required for return flow to occur FIO_MIN 50 absval 8.02 
No.Parameter nameParameterMinimum valueMaximum valueCHG_TYPFitted value
Lateral soil flow coeff-linear adj to daily lateral flow LATQ_CO absval 0.94 
Initial SCS CN II value CN2 −20 20 pctchg −19.04 
Effective hydraulic conductivity in main channel alluvium CHK −0.01 500 absval 9.89 
Groundwater ‘revap’ coefficient REVAP_CO 0.02 0.2 absval 0.2 
Plant water uptake compensation factor EPCO absval 0.323 
Maximum canopy storage CANMX 20 absval 19.89 
Percolation coefficient bottom soil layer due to an impermeable layer or high water table PERCO 0.8 absval 0.97 
Available water capacity AWC −20 20 pctchg −1.62 
Average slope steepness in HRU SLOP 0.01 0.9 absval 0.6 
10 USLE equation support practice (P) factor USLE_P absval 0.32 
11 Threshold depth of water in the shallow aquifer for ‘revap’ to occur REVAP_MIN 50 absval 30.42 
12 Lateral flow travel time LAT_TTIME 0.5 180 absval 110.39 
13 Lag factor for gw recession curve ALPHA absval 0.45 
14 Threshold depth of water in the shallow aquifer required for return flow to occur FIO_MIN 50 absval 8.02 

Note: absval indicates the replacement value, while pctchg indicates the percent change.

Hydro-climatic framework

This framework demonstrates the integration of the GeoMIP6 model with the SWAT+ model, analyzes the application of SRM in tropical basins, and examines the impacts under the SSP2-4.5 and SSP5-8.5 scenarios, as well as the G6solar and G6sulfur scenarios. Figure 2 illustrates four main steps: (1) retrieval of daily precipitation and maximum and minimum temperatures from 1985 to 2100 from the four GeoMIP6 models listed in Table 1 at https://wcrp-cmip.org/cmip-data-access/, followed by bias correction using the LSC approach described in Section GeoMIP6; (2) setup of SWAT+ using observed meteorological, soil, land use and DEM data, along with model calibration and validation with observed streamflow data; (3) analysis of climatic changes at the basin scale using the ensemble mean of the four GeoMIP models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios for the periods of 2025–2044, 2045–2064, and 2065–2084 compared to the 1985–2004 baseline period; and (4) hydrological analysis across the four scenarios and three future scenarios, along with an analysis of spatial changes in different sub-basins.
Figure 2

Hydro-climatic modeling framework for evaluating the impact of SRM in the KRB.

Figure 2

Hydro-climatic modeling framework for evaluating the impact of SRM in the KRB.

Close modal

Bias correction of GEOMIP6

The climatological characteristics of monthly mean precipitation and maximum and minimum temperatures of the KRB from 1985 to 2004, simulated by the selected GeoMIP6 models before and after bias correction, are compared to observed data and shown in Figure 3. The observed data indicated that the highest precipitation occurs in November (399.09 mm) and December (397.33 mm), while the lowest monthly precipitation occurs in February (85.76 mm). The original MPI-ESM1-2-LR and UKESM1-0-LL were unable to accurately simulate the climatology of the KRB, showing peak monthly precipitation in September. In contrast, all the original GeoMIP6 models correctly simulated the lowest precipitation in February, matching the observed value. After bias correction, the climatology characteristics of the four GeoMIP6 models closely match the observed means. These corrected factors were then applied to adjust future climate projections.
Figure 3

Comparison of the climatological characteristics of historical means for (a) monthly precipitation, (b) maximum temperature, and (c) minimum temperature from 1985 to 2004, simulated by both the original and bias-corrected GeoMIP6 models, against observations.

Figure 3

Comparison of the climatological characteristics of historical means for (a) monthly precipitation, (b) maximum temperature, and (c) minimum temperature from 1985 to 2004, simulated by both the original and bias-corrected GeoMIP6 models, against observations.

Close modal

Figure 3 shows that the original GeoMIP6 models underestimated the mean maximum monthly temperature and overestimated the mean minimum monthly temperature compared to the observed data. The temperature differences between the original GeoMIP6 models and observations range from 1 to 4 °C. The peak mean monthly maximum temperature in April, consistent with the observed data, is captured by most of the original models, except for CNRM-ESM2-1, which records it in June. Regarding the mean minimum monthly temperature, the original UKESM1-0-LL failed to capture the peak in April, whereas MPI-ESM1-2-LR recorded the peak 1 month later. After bias correction, most of the models successfully captured the climatological temperature characteristics over the basin. However, UKESM1-0-LL differed from the other three models in terms of the mean minimum monthly temperature, with the highest corrected values in October, while the other models showed the highest values in April. In contrast, the corrected CNRM-ESM2-1 simulated the lowest mean monthly minimum temperature in January, while the other models and observations indicated this occurrence in February. Similar to monthly precipitation, the bias-corrected mean monthly maximum and minimum temperatures now exhibit a closer match with the observed data.

Annual climatic changes

Bias-corrected climate projections were utilized for the following sections, with an ensemble mean of these projections employed to minimize the model uncertainty problem. The temporal changes in annual precipitation and mean maximum and minimum temperatures of the KRB for the ensemble mean across four scenarios, compared to three future and baseline periods, are shown in Figure 4, while their absolute and relative changes are listed in Table 3.
Table 3

A comparison of annual mean precipitation, maximum temperature, and minimum temperature over the KRB under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios

ModelsPrecipitation (%) 2025–2044
Maximum temperature (°C) 2025–2044
Minimum temperature (°C) 2025–2044
G6solarG6sulfurSSP2-4.5SSP5-8.5G6solarG6sulfurSSP2-4.5SSP5-8.5G6solarG6sulfurSSP2-4.5SSP5-8.5
CNRM-ESM2-1 0.31 6.93 2.30 3.43 1.43 1.53 1.41 1.41 0.41 0.80 0.67 0.86 
IPSL-CM6A-LR 1.32 5.51 5.32 10.54 0.23 0.28 0.31 0.01 1.23 1.13 1.37 1.12 
MPI-ESM1-2-LR 10.70 1.74 9.97 17.28 0.24 1.32 0.61 0.15 0.37 0.56 0.16 0.10 
UKESM1-0-LL 4.75 6.19 5.78 6.35 2.14 2.16 2.69 2.61 1.03 0.80 1.06 0.92 
Ensemble mean 4.27 5.09 5.84 9.40 1.01 1.32 1.25 1.04 0.76 0.82 0.81 0.75 
 2045–2064 2045–2064 2045–2064 
CNRM-ESM2-1 1.41 −0.96 −0.91 5.77 1.80 1.96 2.29 2.52 1.51 1.13 1.50 1.80 
IPSL-CM6A-LR 6.70 −1.15 −1.42 2.90 0.53 1.31 1.15 1.16 1.94 1.60 1.54 2.37 
MPI-ESM1-2-LR 30.05 9.55 19.97 30.78 0.13 0.89 0.44 0.09 0.54 0.81 0.61 0.82 
UKESM1-0-LL 12.73 7.02 20.02 17.63 3.06 3.38 3.62 4.24 1.42 0.92 1.21 2.13 
Ensemble mean 12.72 3.62 9.42 14.27 1.38 1.88 1.88 2.00 1.35 1.11 1.21 1.78 
 2065–2084 2065–2084 2065–2084 
CNRM-ESM2-1 −1.28 1.28 4.77 0.61 2.91 2.98 2.62 4.07 2.01 2.31 2.06 3.03 
IPSL-CM6A-LR 1.41 −8.66 6.32 2.85 0.99 1.90 1.20 2.64 1.80 1.78 2.37 2.94 
MPI-ESM1-2-LR 10.85 4.74 9.83 30.71 0.68 0.91 0.90 1.01 0.88 0.90 0.71 1.96 
UKESM1-0-LL −3.38 −8.55 −0.09 −3.98 3.72 3.51 4.15 6.35 2.65 1.89 2.70 4.41 
Ensemble mean 1.90 − 2.80 5.21 7.55 2.07 2.33 2.22 3.52 1.83 1.72 1.96 3.09 
ModelsPrecipitation (%) 2025–2044
Maximum temperature (°C) 2025–2044
Minimum temperature (°C) 2025–2044
G6solarG6sulfurSSP2-4.5SSP5-8.5G6solarG6sulfurSSP2-4.5SSP5-8.5G6solarG6sulfurSSP2-4.5SSP5-8.5
CNRM-ESM2-1 0.31 6.93 2.30 3.43 1.43 1.53 1.41 1.41 0.41 0.80 0.67 0.86 
IPSL-CM6A-LR 1.32 5.51 5.32 10.54 0.23 0.28 0.31 0.01 1.23 1.13 1.37 1.12 
MPI-ESM1-2-LR 10.70 1.74 9.97 17.28 0.24 1.32 0.61 0.15 0.37 0.56 0.16 0.10 
UKESM1-0-LL 4.75 6.19 5.78 6.35 2.14 2.16 2.69 2.61 1.03 0.80 1.06 0.92 
Ensemble mean 4.27 5.09 5.84 9.40 1.01 1.32 1.25 1.04 0.76 0.82 0.81 0.75 
 2045–2064 2045–2064 2045–2064 
CNRM-ESM2-1 1.41 −0.96 −0.91 5.77 1.80 1.96 2.29 2.52 1.51 1.13 1.50 1.80 
IPSL-CM6A-LR 6.70 −1.15 −1.42 2.90 0.53 1.31 1.15 1.16 1.94 1.60 1.54 2.37 
MPI-ESM1-2-LR 30.05 9.55 19.97 30.78 0.13 0.89 0.44 0.09 0.54 0.81 0.61 0.82 
UKESM1-0-LL 12.73 7.02 20.02 17.63 3.06 3.38 3.62 4.24 1.42 0.92 1.21 2.13 
Ensemble mean 12.72 3.62 9.42 14.27 1.38 1.88 1.88 2.00 1.35 1.11 1.21 1.78 
 2065–2084 2065–2084 2065–2084 
CNRM-ESM2-1 −1.28 1.28 4.77 0.61 2.91 2.98 2.62 4.07 2.01 2.31 2.06 3.03 
IPSL-CM6A-LR 1.41 −8.66 6.32 2.85 0.99 1.90 1.20 2.64 1.80 1.78 2.37 2.94 
MPI-ESM1-2-LR 10.85 4.74 9.83 30.71 0.68 0.91 0.90 1.01 0.88 0.90 0.71 1.96 
UKESM1-0-LL −3.38 −8.55 −0.09 −3.98 3.72 3.51 4.15 6.35 2.65 1.89 2.70 4.41 
Ensemble mean 1.90 − 2.80 5.21 7.55 2.07 2.33 2.22 3.52 1.83 1.72 1.96 3.09 

Bold text denotes significance at the 0.05 level.

Figure 4

The temporal changes in the multi-model ensemble mean of annual precipitation (Pr), maximum temperature (Tmax), and minimum temperature (Tmin) of the KRB from 1980 to 2085 under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Figure 4

The temporal changes in the multi-model ensemble mean of annual precipitation (Pr), maximum temperature (Tmax), and minimum temperature (Tmin) of the KRB from 1980 to 2085 under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Close modal

The ensemble mean projected an increasing trend in annual precipitation in the middle of the 21st century, followed by a decreasing trend toward the end of the 21st century under the evaluated emission scenarios, except for the G6sulfur scenario, which shows a continuous decrease in precipitation from 2025 to 2084 (Figure 4 (a)–(d)). In particular, the reduction in precipitation is most pronounced under the two G6 scenarios, with the G6sulfur scenario showing the greatest decrease (slope = −8.32). The precipitation projections from the four models are consistent with previous studies, indicating a reduction in mean precipitation when compared to the SSP5-8.5 scenario (Henry & Mendonca 2020). The drier conditions projected under the G6sulfur scenario are particularly evident in the 2065–2084 period, as indicated by the IPSL-CM6A-LR and UKESM1-0-LL models, with a decrease of up to 8.66% as detailed in Table 3. The mean annual precipitation is projected to increase by 7.55–14.27% under the SSP5-8.5 scenario. These increases could be reduced by 1.9 to 12.72%, −2.8 to 5.09%, and 5.21 to 9.42% under the G6solar, G6sulfur, and SSP2-4.5 scenarios, respectively. CNRM-ESM2-1 and IPSL-CM6A-LR projected decreases of annual precipitation in the 2045–2064 period under the SSP2-4.5 and G6sulfur scenarios, while UKESM1-0-LL projected decreases across all four emission scenarios in the 2065–2084 scenario. Overall, based on the ensemble mean, the total precipitation in most scenarios remains higher than the historical levels (1985–2004), except for the G6sulfur scenario in 2065–2084, which shows a slight decrease compared to the historical period.

Simultaneously, the multi-model ensemble mean shows a substantial increasing trend in annual maximum and minimum temperatures over the KRB from 2025 to 2084, particularly under the SSP5-8.5 scenario (Figure 4). Under the SSP5-8.5 scenario, there is a notable rise in both maximum and minimum temperatures, ranging from 1.04 to 3.52 and 0.75 to 3.09 °C, respectively (Table 3). The G6solar and G6sulfur scenarios limit the dramatic increases in maximum temperature projected under SSP5-8.5, ranging from 1.01 to 2.07 and 1.31 to 2.33 °C, respectively. For minimum temperature, these scenarios also limit the increases compared to SSP5-8.5, ranging from 0.76 to 1.83 °C (G6solar) and 0.82 to 1.72 °C (G6sulfur). These changes in maximum and minimum temperatures under SRM correspond closely with those under SSP2-4.5, ranging from 1.25 to 2.22 and 0.81 to 1.96 °C, respectively. In the SSP5-8.5 scenario, the temperature rise is driven by a significant increase in greenhouse gas concentrations in the atmosphere. In contrast, the SRM scenario mitigates this temperature increase by reducing climate forcing through human intervention. The primary cause of the cooling effect from SRM is the reflection of shortwave radiation back to space by the aerosols that are injected into the stratosphere. While this process helps to reduce the intense solar radiation reaching the equatorial region and consequently lowers temperatures, the increases remain below those observed in the SSP5-8.5 scenario.

Monthly climatic changes

Figure 5 illustrates the relative changes in monthly mean precipitation from the multi-model ensemble mean across four different scenarios, compared to the baseline period of 1985–2004. During 2025–2044, from November to April under SSP2-4.5 and SSP4-8.5, and from November to May under G6solar and G6sulfur, the monthly mean precipitation in the multi-model ensemble mean exceeds that of the baseline period. Especially notable is the increase in monthly mean precipitation in February, which ranges from 39.78% (G6sulfur) to 66.09% (SSP5-8.5) compared to the baseline period. A possible explanation for this change is that the MPI-ESM1-2-LR and UKESM1-0-LL models exhibit significantly higher precipitation compared to the other two models during this period. In 2045–2064, each scenario exhibits distinct variations, with the highest increase in precipitation observed in January for G6solar, showing a 46.95% rise compared to the baseline period. In contrast, the other three scenarios experience their greatest increase in precipitation in November, ranging from 38.59% (G6sulfur) to 46.32% (SSP5-8.5). This phenomenon indicates that the flood risk in the KRB rises during the rainy season. During the 2065–2084 period, the only consistent trend across all scenarios is a decrease in December precipitation, ranging from 5.20% (G6solar) to 9.98% (G6sulfur). There is also a decrease in monthly mean precipitation under G6sulfur during the low precipitation months from February to May in the periods of 2045–2064 and 2065–2084. This finding suggests that this SRM strategy could potentially worsen the water shortage issue in the KRB.
Figure 5

Relative changes in monthly mean precipitation of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Figure 5

Relative changes in monthly mean precipitation of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Close modal

When comparing the four models, UKESM1-0-LL stands out from the other models in most of the evaluated periods and scenarios. For example, in 2025–2044, except for UKESM1-0-LL, the other three models exhibit minor fluctuations compared to the baseline period. From December to April, there is an increase in monthly mean precipitation in UKESM1-0-LL, followed by a decrease from June to October. The most significant increase in precipitation during this period exceeds 100% of the baseline period, particularly in February. From June to October, there is a reduction in monthly mean precipitation compared to the baseline period, with the most significant reduction in July across all scenarios, ranging from 48.72 to 58.31%. MPI-ESM1-2-LR shows more precipitation over the spring season under certain scenarios, such as G6solar during 2045–2064, where the monthly mean precipitation in February is 241.26% greater than the baseline period. In the period of 2065–2084, UKESM1-0-LL projected an increase in monthly mean precipitation from February to August, while the other three models show a decrease in precipitation. UKESM1-0-LL shows a decrease in monthly mean precipitation from September to January, while the other three models show an increasing trend. In the MPI-ESM1-2-LR model, monthly mean precipitation under SSP5-8.5 shows an increase from January to April, with the most substantial increase in February, which is 163.37% greater than the baseline period. In summary, the precipitation simulations for the KRB from the UKESM1-0-LL and MPI-ESM1-2-LR models exhibit significant inconsistencies, potentially exacerbating extreme precipitation events.

Figure 6 illustrates the absolute changes in monthly mean maximum temperature in the multi-model ensemble mean compared to the 1985–2004 baseline period across the KRB. In each scenario, a consistent trend emerges, with the most significant temperature rise occurring in 2065–2084, followed by 2045–2064 and 2025–2044. Decreases of monthly mean maximum temperature occur in April and May during the 2025–2044 period, with the greatest reduction under G6solar. In 2045–2064, the smallest temperature increases occur from February to April, with March being particularly notable under G6solar. The most significant temperature rises, however, occur in August and September. In 2065–2084, SSP5-8.5 exhibits much higher values compared to the other three scenarios. The smallest increases are observed in April and September, while the most substantial rises occur in December and January. The temperature rise in G6solar is relatively lower than the other three scenarios.
Figure 6

Absolute changes in the monthly mean maximum temperature of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Figure 6

Absolute changes in the monthly mean maximum temperature of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Close modal
Figure 7

Absolute changes in the monthly mean minimum temperature of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Figure 7

Absolute changes in the monthly mean minimum temperature of the KRB across four GeoMIP6 models under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Close modal

Regarding model uncertainty, the increases and decreases in monthly mean maximum temperature for UKESM1-0-LL remain the most significant across the models. In the period of 2025–2044, it shows a notably larger temperature rise compared to the other three models from August to January and also the lowest value in April and May, as shown in Figure 6. In 2045–2064, the temperature variation of UKESM1-0-LL is consistently higher than that of the other three models from December to May. During the 2065–2084 period, it shows a larger temperature rise from November to March. MPI-ESM1-2-LR demonstrates the smallest increases in monthly mean maximum temperature across all scenarios, occasionally even displaying negative changes.

The multi-model ensemble mean projected the greatest increases in monthly mean minimum temperature during the 2065–2084 period across all four emission scenarios, as shown in Figure 7, similar to the trends in the monthly mean maximum temperature. In the 2025–2044 period, the monthly mean minimum temperature shows a significant rise at the start and end of the year. The smallest increase is observed in July under G6sulfur and in June for the other three scenarios, with increases ranging from 0.79 to 0.87 °C. The monthly mean minimum temperature is projected to increase moderately during the 2045–2064 period, ranging from 1.61 to 2.32 °C. In contrast, the 2065–2084 period records the highest rise in monthly mean minimum temperature in March, ranging from 3.09 to 4.57 °C. Meanwhile, the smallest temperature increases occur in September, ranging from 1.73 to 3.04 °C. The temperature variations observed during the 2025–2044 and 2065–2084 periods can largely be attributed to the influence of UKESM1-0-LL, particularly its decline seen in June during the 2025–2044 period. Meanwhile, the monthly mean minimum temperature had a substantial rise during the 2065–2084 period. A comparison among models reveals notable regional variations in simulation outcomes when considering climate change within the context of geoengineering scenarios (Cao et al. 2017).

Hydrological temporal changes

The temporal changes in observed and simulated monthly streamflow for the KRB, as simulated by SWAT+ at the Jambatan Guillermard station from 1985 to 2004, are shown in Figure 8. The NSE and R2 values for the calibration period were both 0.83, while, for the validation period, they were 0.66 and 0.76, respectively. Over the entire simulation period, the NSE value was 0.76 and the R2 value was 0.78, indicating that the performance of SWAT+ is considered good. The peak simulated streamflow is generally consistent with the peak observed streamflow. However, from 2000 to 2005, the simulated monthly mean streamflow was slightly higher than the observed monthly mean streamflow, mainly due to the lack of groundwater data, which is one of the major freshwater sources in the KRB (Hussin et al. 2020).
Figure 8

The calibration and validation of SWAT+ for simulating monthly streamflow from 1985 to 2004 at the Jambatan Guillermard station.

Figure 8

The calibration and validation of SWAT+ for simulating monthly streamflow from 1985 to 2004 at the Jambatan Guillermard station.

Close modal
The temporal changes in annual mean streamflow at the Jambatan Guillermard station in the KRB from 1985 to 2084 are shown in Figure 9. The annual mean streamflow for the multi-model ensemble mean from 1985 to 2004 was 401.75 m3/s. From 2025 to 2084, GeoMIP6 projections indicate that SSP2-4.5 and SSP5-8.5 exhibit the highest future streamflow, with mean streamflow rates of 490.48 and 512.78 m3/s, respectively. The SSP2-4.5 scenario has the second-highest streamflow, while G6sulfur exhibits the lowest streamflow at 408.40 m3/s. In terms of shifting patterns, except for the G6sulfur scenario, monthly streamflow across the other three models is projected to increase to varying extents compared to the baseline period.
Figure 9

Temporal changes of annual streamflow from 1985 to 2084 at the Jambatan Guillermard station based on the multi-model ensemble mean.

Figure 9

Temporal changes of annual streamflow from 1985 to 2084 at the Jambatan Guillermard station based on the multi-model ensemble mean.

Close modal
Figure 10 presents the relative changes in monthly mean streamflow at the Jabatan Guillermard station within the KRB. This analysis covers across four emission scenarios and three time periods, compared to the 1985–2004 baseline period. In general, the streamflow changes closely follow the precipitation change patterns as shown in Figure 5. Four key findings from Figure 10 include: (1) the increase in monthly mean streamflow in the 2025–2044 period, particularly from February to May, is generally higher than in the other two periods; (2) the increase in monthly mean streamflow during the heavy precipitation months, especially in November and December, is greater in the 2045–2064 period than in the other two periods; (3) the decline in monthly mean streamflow is predominantly projected under G6sulfur during the 2045–2064 period; and (4) the greatest model uncertainty is found in the UKESM1-0-LL model during both the 2025–2044 and 2065–2084 periods, whereas the MPI-ESM1-2-LR model exhibits higher uncertainty in the 2045–2064 period. Although precipitation was the primary factor affecting streamflow variations during the 2065–2084 period, the simulation results from each model revealed considerable inconsistency, suggesting that temperature also played a significant role in influencing streamflow.
Figure 10

Relative changes of monthly mean streamflow at the Jambatan Guillermard station in the KRB across three future periods under the SSP and SRM scenarios.

Figure 10

Relative changes of monthly mean streamflow at the Jambatan Guillermard station in the KRB across three future periods under the SSP and SRM scenarios.

Close modal

Hydrological spatial changes

Figure 11 illustrates the spatial distribution of annual mean streamflow changes in the KRB, projected by the multi-model ensemble mean across four emission scenarios and three future periods. There is a general increase in annual mean streamflow across the basin during the 2025–2044 period, with a more significant increase observed downstream, particularly under SSP5-8.5. During the 2045–2065 period, a general increase in annual mean streamflow is seen compared to the 2025–2044 period, particularly under the G6solar and SSP5-8.5 scenarios. However, some decreases in annual mean streamflow are observed in the middle part of the basin under SSP2-4.5, with the smallest increment occurring under G6sulfur. In the 2065–2084 period, a significant decrease in streamflow is observed under G6sulfur, especially in the middle and upper parts of the basin. This aligns with the findings of Tan et al. (2024), who reported that G6sulfur could bring a drier condition in the Muda River Basin compared to G6solar. G6sulfur involves injecting sulfate aerosols into the stratosphere, similar to the effect of large volcanic eruptions, to reflect solar radiation and cool the planet. However, these particles can also alter atmospheric circulation and cloud formation and reduce evaporation due to cooler conditions.
Figure 11

Relative changes of the annual mean streamflow at the sub-basin level of the KRB by the multi-model ensemble mean under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Figure 11

Relative changes of the annual mean streamflow at the sub-basin level of the KRB by the multi-model ensemble mean under the SSP2-4.5, SSP5-8.5, G6solar, and G6sulfur scenarios.

Close modal

This study employs four GeoMIP6 models and SWAT+ to evaluate the impact of SRM on hydro-climatic changes in the KRB, Malaysia, using a baseline period from 1985 to 2004 and three future periods of 2025–2044, 2045–2064, and 2065–2084, Four distinct scenarios are considered, including two SRM scenarios (G6solar and G6sulfur) and two Shared Socioeconomic Pathways (SSP2-4.5 and SSP5-8.5). The main findings of this study are as follows:

  • The original MPI-ESM1-2-LR and UKESM1-0-LL models were unable to accurately capture the peak monthly precipitation in the KRB. Additionally, all four GeoMIP6 models showed an underestimation of maximum temperature and an overestimation of minimum temperature. The LSC approach is effective in reducing biases in precipitation and temperature within the original GeoMIP6 models, bringing them into closer alignment with the observations.

  • G6solar and G6sulfur demonstrate effective cooling effects on both maximum and minimum temperatures, thereby limiting the temperature rise projected under SSP5-8.5, which could reach up to 3.52 °C by the end-21st century. This aligns with the temperature projections of SSP2-4.5. Monthly maximum and minimum temperatures are projected to increase in almost all the evaluated periods, except in April and May in the 2025–2044 period. This situation is attributed to the decrease in monthly temperature as projected by UKESM1-0-LL. Additionally, MPI-ESM1-2-LR demonstrates the most modest temperature increases compared to the other three models.

  • The multi-model ensemble mean projected an increasing trend in annual precipitation from the early to mid-21st century, followed by a decline toward the end of the 21st century under SSP2-4.5, SSP5-8.5 and G6solar, while G6sulfur shows an overall decreasing trend over the same period. In general, annual precipitation in the KRB is projected to increase in the future compared to the baseline period, except for G6sulfur, which showed a decline in the 2065–2084 periods. The decreases in monthly precipitation under G6sulfur, particularly during the dry months, suggest that this strategy may exacerbate the water shortage issue in the KRB.

  • The highest increase in mean annual streamflow is projected by SSP5-8.5, followed by SSP2-4.5, G6solar, and G6sulfur. In the 2025–2044 period, the increases in monthly streamflow are generally higher during the dry months from February to May compared to the other two periods. In contrast, the rise in monthly streamflow is higher during the 2045–2064 period, showing the potential for serious flooding in the mid-21st century in the KRB. Decreases in monthly streamflow were projected in the 2045–2064 period under G6sulfur, particularly in the middle and upper parts of the basin.

However, some limitations need to be addressed in future studies. MPI-ESM1-2-LR and UKESM1-0-LL show greater uncertainties compared to the other two models in the KRB. The model uncertainties may arise from factors such as model structure, regional topography, and atmospheric circulation (Ongoma et al. 2018; Berhanu et al. 2023; Xiao et al. 2023), where differences in initial and boundary conditions, along with the poor representation of convective schemes and model parameterizations, hinder models from capturing precipitation spatial patterns accurately. Climate models that are unable to accurately represent the climate system in the study area may not contribute to improvements in the ensemble mean (Berhanu et al. 2023). While the ensemble mean from a certain number of climate models is commonly accepted as a widely used approach to minimize the model uncertainty, it may not significantly enhance projection capabilities. The upcoming GeoMIP7 should include more climate models and climate variables, such as precipitation and maximum and minimum temperatures, that are suitable for running hydro-climatic modeling at the basin scale. This would allow the selection and ensemble of more appropriate climate models, thereby increasing the robustness of the findings.

Both G6solar and G6sulfur involve the artificial injection of aerosols into the stratosphere or the reduction of the solar constant in the model. Furthermore, there are uncertainties in stratospheric dynamics, such as radiative interactions and stratospheric chemistry interactions, which influence local radiation transmission, leading to varied local heating of the atmosphere and consequent impacts on surface climate and the stratosphere (Niemeier & Schmidt 2017; Kleinschmitt et al. 2018). Consequently, model simulations may not be as useful in reducing some uncertainties. New experiments should be designed to enhance the accuracy of modeling interactions in the atmosphere or improve model parameters for regional-scale simulations.

The SWAT+ model tends to overestimate low flows in the KRB, possibly due to the plant growth and land use models in the SWAT being developed for temperate regions, which differ from the characteristics of tropical regions like Malaysia (Strauch & Volk 2013; Tan et al. 2017a). In this study, hydrological data were solely sourced from a single site, lacking validation at multiple sites. Further investigation is required to determine if integrating groundwater and soil moisture data may enhance the reliability of SWAT+. CMIP6 models are primarily available at global and continental scales (Tan et al. 2020). Before applying them to local-scale assessments, downscaling to finer scales can increase the reliability of future climate assessments (Tan et al. 2020). Improvements in model resolution may also aid in more accurately simulating precipitation (Berhanu et al. 2023). Thus, it would be great to consider employing more robust downscaling techniques (Duan et al. 2017) or possibly include some GeoMIP models in the CORDEX-SEA downscaling initiatives for future SRM hydro-climatic studies.

This research was funded by the Ministry of Higher Education Malaysia through the Long-term Research Grant Scheme Project 2 (Grant No. LRGS/1/2020/UKM-USM/01/6/2), as part of the program of LRGS/1/2020/UKM/01/6. Additional support for this work was provided by the Degrees Initiative (Grant No. RGA-DMF23MYS). L.X. is supported by the US National Science Foundation (Grant No. AGS-2017113). The authors extend their gratitude to the editors and reviewers for their valuable and constructive comments, which have greatly improved this manuscript.

H.D. carried out methodology, software, validation, formal analysis and wrote the original draft preparation. M.L.T. performed conceptualization, supervision, data curation, visualization, project adminstration, funding acquisition, and wrote the reviewed and edited the manuscript. L.X. wrote the reviewed and edited manuscript. Y.L.T. performed data curation. Z.M.Y. wrote the reviewed and edited manuscript.

All relevant data are included in the paper or its Supplementary Information.

The authors declare there is no conflict.

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