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Research Article

Applicability of SWOT data in calibrating WRF-Hydro hydrological model over the Tawa River basin

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Article: 2185292 | Received 11 Oct 2022, Accepted 22 Feb 2023, Published online: 06 Mar 2023

Abstract

Freshwater is considered an essential natural resource that must be monitored effectively. The Surface Water and Ocean Topography (SWOT) satellite mission scheduled for launch in December 2022 will enable river discharge estimation from surface water extents, elevations, and slopes. However, the SWOT-based discharges will be inconsistent due to infrequent temporal sampling (TS) of SWOT orbit. This study explores the potential of unique TS of SWOT to determine whether it influences the calibration of hydrological model. The Weather Research and Forecast Hydrological system (WRF-Hydro) has been used to simulate river discharge. Further WRF-Hydro model has been calibrated using proxy SWOT data based on a dynamically dimensioned search algorithm. Results show that more than 90% of parameter iterations have KGE values with less than 20% absolute percent difference when only SWOT TS alone has been considered. The results suggest that model calibration using SWOT-based discharge performs similarly to daily in-situ discharge.

1. Introduction

Understanding the dynamics of river discharge is crucial for hydrological applications like water resource allocation and flood risk management (Jongman et al. Citation2012; Durand et al. Citation2014; Kansakar and Hossain Citation2016). Hydrological models such as Weather Research and Forecast Hydrological system (WRF-Hydro) have the potential to comprehend and access the transport of water, thereby serving applications like flood forecasting (Andreadis and Schumann Citation2014). In recent years, WRF-Hydro has expanded into a more versatile coupling architecture for integrating hydrological and atmospheric models. Coupled with fine-scale hydro-meteorological models, WRF-Hydro can estimate runoff, streamflow, and flood forecasts at grid resolutions of a few kilometers or less (e.g. (Yucel et al. Citation2015; Senatore et al. Citation2015; Arnault et al. Citation2016). However, parameter calibration of WRF-Hydro is crucial for accurately simulating the observed runoff process, including those governing the channel’s total water volume and discharge distribution. Hence, to ensure superior performance by hydrologic models, in-situ observations are quintessential for the calibration process, such as river discharge (Sun et al. Citation2012).

Unfortunately, quantifying in-situ discharge measurement is not possible for a variety of reasons, including the dispersed location of gauge stations (Vorosmarty et al. Citation2001) or owing to the lack of data sharing policy among the neighboring nations (Biancamaria et al. Citation2011; Hossain et al. Citation2014). The potential reason for scarcity in discharge measurements is sometimes lack of resources for the deployment of in-situ gauges (Hrachowitz et al. Citation2013), especially in ungauged basins or remote areas. Also, the nation’s contentious water policy results in a lack of measurement transparency (Gleason et al. Citation2018). Furthermore, the deployment of man-made obstructions such as dams have altered the natural flow regime of rivers to such an extent that the historical gauging stations, which had a more extended period of discharge measurement, are no longer applicable for analyzing current river dynamics (Pinter et al. Citation2008; Hossain et al. Citation2014; Wu et al. Citation2018). As a result, there is a need to investigate alternative ways of determining river discharge in addition to field measurements.

Remotely sensed satellite observations have a great advantage over in-situ observations in terms of spatial coverage and global accessibility (Alsdorf and Lettenmaier Citation2003). The remotely sensed satellite observations are not intended to replace in-situ gauge stations but rather to complement existing data collections (Alsdorf et al. Citation2003; Papa et al. Citation2010; Hossain et al. Citation2014; Thakur et al. Citation2021; Verma et al. Citation2021; Dhote et al. Citation2021). Unfortunately, neither a satellite nor an airborne sensor can directly measure the river discharge; rather, the river discharge can be estimated from remotely sensed hydrologic observables such as surface water extent and elevations (Bjerklie et al. Citation2003; Smith and Pavelsky Citation2008; Gleason and Smith Citation2014; Durand et al. Citation2016; Tarpanelli et al. Citation2017).

In the past two decades, satellite altimetry has shown great potential in observing surface water elevations, despite its limited spatial coverage due to its nadir look and 10- to 35-day revisit time (JASON and SARAL/AltiKa, respectively) (Verma and Indu Citation2021). Previous studies have tried to reduce the revisit cycles and spatial coverage of altimetry by combining multi-missions, but this further led to an additional challenge of bias correction of incongruent orbital cycles of different altimetry missions for observed space in time (Crétaux et al. Citation2015; Tarpanelli et al. Citation2017; Bjerklie et al. Citation2018). So, until the Surface Water and Ocean Topography (SWOT) mission, which was launched in December 2022, the desired requirement for studying surface water elevations and extent, along with enhanced sampling frequency by a single satellite was still distinct. Due to its wide swath of 120 km, the SWOT will globally observe both surface water elevation and extent (Biancamaria et al. Citation2016; Nair et al. Citation2022). The SWOT measurements such as river width, elevation, and slopes have been used to derive river discharge and associated uncertainties in many previous studies (Gleason and Smith Citation2014; Garambois and Monnier Citation2015; Durand et al. Citation2016; Bonnema and Hossain Citation2017; Hagemann et al. Citation2017), but very few studies analyzed the irregular Temporal Sampling (TS) of SWOT orbit (Nickles et al. Citation2020). Pedinotti et al. (Citation2014) demonstrate how satellite remote sensing, coupled with hydrologic models, improves discharge estimation. Elmer et al. (Citation2020) investigate how data assimilation is an alternative method for incorporating remotely sensed observations into models for discharge estimation, which would be important for SWOT-observed data. Huang et al. (Citation2020) calibrated a hydrologic model using SWOT-like observations in ungauged basins and obtained a 0.85 Nash–Sutcliffe Efficiency. The study utilized Landsat-derived river widths and in-situ water levels to create SWOT observations. Even though these studies accurately represent SWOT-like observations, but they don’t examine whether SWOT's infrequent temporal sampling frequency would effectively perform hydrologic model calibration. So, the research is needed to identify the potential role of SWOT TS discharge versus daily discharge in calibrating hydrological models without data assimilation.

Even though the SWOT mission will enhance the spatial coverage, unlike current altimetry missions and in-situ gauge stations, SWOT observations are irregular (2 to 6 times observation) depending on the latitude within 21 days of the repeat orbit (Pavelsky et al., Citation2014)(Pavelsky et al. 2014). The present study examines the research hypothesis: “Will SWOT measurements be useful in hydrological model calibration to improve model performance? This study focuses on identifying the potential role of SWOT temporal sampled discharge relative to daily discharge in calibrating hydrological models. The objective is to determine whether irregular TS-based SWOT discharge may replace daily in-situ observed discharge in future WRF-Hydro hydrological model calibration.

2. Materials and methods

2.1. Study area

Tawa River is the longest (172 km) tributary of the Narmada River and drains through India’s Hoshangabad district of Madhya Pradesh state. Tawa dam is situated across the Tawa River at a latitude of 22030’40” N and a Longitude of 77056’30” E, which is a significant irrigation project in the state and covers a catchment area of about 6000 km2 (). The dominant soil type of the region is black alluvium and ferruginous red ravel, also called “black cotton.” The black-cotton soil has excellent porosity and moisture retention capability, making the region highly argillaceous. The region’s climatology can be majorly categorized into three seasons; pre-monsoon (March-April-May), post-monsoon (October-November-December), with nearly no rainfall, and monsoon (June-July-August-September), with an annual mean rainfall of about 550 mm. The monthly mean temperature ranges from 12° C (minimum temperature) to 42° C (maximum temperature). So, the water level of the Tawa dam provides crucial information to water managers to regulate the dam’s outflow, which is majorly dependent on the rainfall during the monsoon and inflows from the upstream river. In , the WRF-Hydro domain (legend denoted as study domain) for the current study covers a large area of 65000 km2, which also covers the streamflow of the tributaries coming from the east. Consequently, the output of the model at the Hoshangabad gauge station takes into account the flow of the large tributary flowing from the east. So, the model out at the Hoshangabad gauge station also considers the flow in tributary coming from the east. Also, the gauging station location corresponds to the outlet of the modeled watershed in the study.

Figure 1. Map of study area representing study domain, Hoshangabad gauge station location, SWOT calibration and validation orbital pass over the Narmada River.

Figure 1. Map of study area representing study domain, Hoshangabad gauge station location, SWOT calibration and validation orbital pass over the Narmada River.

2.2. Data used

In the current study, in-situ observed daily discharge data at the Hoshangabad gauging station monitored by the Centre Water Commission (CWC) of India have been used from 1 January 2011 to 31 December 2017. Furthermore, for calibration, three types of discharge data have been used. First is the in-situ observed or gauge discharge data (hereinafter referred to as Qg) downloaded from the Indian Water Resource Information System (India-WRIS) web portal. The second discharge data is based on the temporal revisit of SWOT (hereinafter mentioned as Qgt), which is the subset of Qg when the SWOT satellite passes over the gauging station. For the extraction of Qgt from Qg, the orbital pass and temporal cycle over the gauging station have been simulated using CNES Large-Scale Hydrology Simulator (https://github.com/CNES/swot-hydrology-toolbox). The third discharge data is SWOT-like data (Qs) derived by following the Qgt considering uncertainty associated with the SWOT discharge algorithm, defined in Hagemann et al. (Citation2017).

2.3. WRF-Hydro model calibration

WRF-Hydro is fully distributed with multi-physics and multi-scale capabilities, enabling it to represent processes on various spatial scales (Yucel et al. Citation2015; Senatore et al. Citation2015; Arnault et al. Citation2016). The WRF-Hydro modeling system version 5.1.1 has been used in the study. The WRF-Hydro system contains several components of the distributed hydrological process and channel flow (Lahmers et al. Citation2019). WRF-Hydro and Noah-MP exhibit parameters often remain dependent on land use (i.e. vegetation density and type) and soil type (i.e. silt, clay, loam, sand). The calibration process determines the optimal coefficient values applied to parameters in the spatial domain. As suggested by Yucel et al. Citation2015; Verri et al. Citation2017; Rummler et al. Citation2019; Camera et al. Citation2020, four parameters that are most sensitive to discharge were calibrated namely: (i) soil permeability or runoff infiltration (REFKDT), (ii) surface retention depth (RETDEPRTFAC), (iii) overland flow roughness factor or surface runoff (OVROUGHTFAC), and (iv) Manning’s factor for channel roughness (MannN). The reference values have been provided in .

Table 1. WRF-Hydro calibration parameter, definition, and scaling factor ranges considered in calibration process.

The calibration procedure is based on the Dynamically Dimensioned Search (DDS) algorithm designed by Tolson and Shoemaker (Citation2007). The DDS is a simple, heuristic, single-solution-based global search algorithm developed to find approximated globally optimal solutions within the specified range of function evaluations (Tolson and Shoemaker Citation2007). The algorithms start with the global search and gradually progress towards the local search while approaching a maximum allowable number of the model iterations. The gradual transition from global to local search exhibits dynamic adjustment to the search dimension, and the parameters’ dimensionality changes. The algorithm randomly selects the parameters with the best solution of the current model iteration and slightly distributes them to generate a revised candidate solution in the next iteration. DDS is, therefore, not designed to cover the global optimum precisely; however, it covers the regional global optimum in the best case and good local optimum in the worst-case scenarios (Tolson and Shoemaker Citation2007).

For the experiment, model iteration has been performed using a combination of four parameter values chosen by the DDS algorithm within the predefined range tabulated in . The error matric in each iteration has been calculated by comparing the WRF-Hydro model output (Qw) with Qg, Qgt, and Qs, respectively. The aim is to see the impact on the model calibration with respect to different discharge time series concerning infrequent TS of the SWOT mission. Since the SWOT mission’s planned designed life is for three years, calibration of WRF-Hydro model simulations have been performed from the year 2015 to 2017 with one year of model spin-up. WRF-Hydro model output was calibrated at the Hoshangabad gauge station, which had consistent daily data from 2011 to 2017. Furthermore, to access the performance of each set of parameters, Kling-Gupta efficiency (KGE) (Gupta et al. Citation2009) has been calculated between the Qw and each of three time-series (Qg, Qgt, and Qs) respectively (). Where, the KGE is defined in EquationEquation 1. (1) KGE=1 (r1)2+(β1)2+(γ1)2(1)

Figure 2. Methodology flowchart for calibrating WRF-Hydro model using DDS algorithm.

Figure 2. Methodology flowchart for calibrating WRF-Hydro model using DDS algorithm.

Where; r= cov(Qm,Qo)σQmσQo; β= μQmμQo; γ= σQm/μQmσQo/μQo

Where r is the correlation coefficient, β is the bias ratio, and γ is the relative variability between the time series such Qw and one of three times series (Qg, Qgt, and Qs). Also, µ, and σ denotes the mean and standard deviation of the time series. A KGE value closer to 1 represent the model output accuracy with respect to the in-situ value (Knoben et al. Citation2019).

The entire watershed contained shallow to medium-depth alluvium formations, both recent and old. The dominant soil type of the region is black alluvium and ferruginous red ravel, also called “black cotton.” The black-cotton soil has excellent porosity and moisture retention capability, making the region highly argillaceous. The study area is located in the north, and forest cover can be seen along the foothills of India’s Satpura range. The slope is generally steep in the foothills of the Satpura range but moderate to gentle towards the Narmada River (Malik and Shukla Citation2015). Because of good irrigation sources and fertile alluvial soil, the entire catchment area is rich in agriculture. Agricultural land accounts for nearly 90% of the watershed basin’s total area. The Satpura range’s foothills are covered in forest. There are also some patches of scrub land near both banks of the Tawa River (Malik and Shukla Citation2015). This land use and land cover class may greatly influence the MannN parameter. Based on previous studies, Chen (Citation2007) has suggested that the REFKDT parameter controls the hydrograph volume. Also, the increment in the REFKDT factor by 0.1 considerably impacts the surface runoff.

Similarly, the REFKDT range in the current study is also considered from 0.5 to 1.5 with an increment factor of 0.1. Hence, it was anticipated that the infiltration and surface retention depth were more sensitive to KGE values than other parameters. In the WRF-Hydro modeling system, the available streamflow input water is derived mainly from the amount of precipitation in infiltration capacity excess in each model grid (Ryu et al. Citation2017). It can also be inferred from (Dubey et al. Citation2021) that when soil condition is unsaturated, higher is the REFKDT value and smaller is the simulated volume. Also, the increment in REFKDT decreases surface runoff. This supports the assertion that REFKDT values are significantly high when the soil is unsaturated during non-monsoon or low-flow conditions.

3. Results and discussion

The WRF-Hydro parameters and corresponding relationship with KGE values have been shown in . In , we can see that the best model iteration based on optimal parameters was selected by the DDS algorithm concerning different target discharge Qg in , Qgt in , and Qs in during the calibration stage. The DDS algorithm arbitrarily selected the initial parameter values during the global search phase. However, as the number of iterations increased, the negative KGE values improved during the local search phase, along with the reduction in the randomness of parameters.

Figure 3. WRF-Hydro model calibration performance using KGE for different normalized parameter values obtained by the best iteration of the DDS algorithm targeting the different discharge: (a) Qg, (b) Qgt, and (c) Qs. The x-axis represents the best model iteration, the left vertical axis represents the model performance by KGE, and the right vertical axis represents the normalized values of parameters selected by the DDS algorithm for calibrating the model. The normalized values of parameters have been shown to represent better parameter values having varied scales.

Figure 3. WRF-Hydro model calibration performance using KGE for different normalized parameter values obtained by the best iteration of the DDS algorithm targeting the different discharge: (a) Qg, (b) Qgt, and (c) Qs. The x-axis represents the best model iteration, the left vertical axis represents the model performance by KGE, and the right vertical axis represents the normalized values of parameters selected by the DDS algorithm for calibrating the model. The normalized values of parameters have been shown to represent better parameter values having varied scales.

The parameters such as surface infiltration (REFKDT) and surface retention depth (RETDEPRTFAC) are more sensitive towards the KGE than other parameters. In , the slight variation of a 0.07 scaling factor in surface retention depth and a 2-scaling factor change in surface infiltration impact KGE values ranging from −1 to 0.65 by 24 model iterations. It can be observed that when the soil is unsaturated during non-monsoon or low-flow conditions, the REFKDT values are much higher. However, with the increment in the REFKDT scaling factor, the hydrograph becomes much smoother due to a decrease in surface runoff which further affect the KGE values. Similarly, the roughness parameters such as OVROUGHRTFAC and MannN control the speed of streamflow in the channel network. The MannN parameter scaling factor’s linear increment increases the KGE values. However, the OVROUGHRTFAC parameter scaling factor decreases the KGE values due to the prolonged confluence time of surface runoff. In , since the Qgt has been derived from Qg, it can be observed that the comparison between the model calibration based on Qg and Qgt has no significant difference in normalized parameter range and KGE values. However, the model calibration based on Qs has a slight skewness in the KGE values towards the right (). Also, a slight discrete pattern in parameter selection has been observed during the local search of the DDS algorithm. So, it can be observed that the calibration targeting Qg derived from infrequent TS of SWOT has no significant effect on optimizing best parameters in fewer model iterations than Qs. Also, the calibration performance of Qgt in terms of KGE values was found to be better than Qs. Overall, the DDS algorithm has converged the parameter values to the best performance level of KGE at the Hoshangabad gauge station shown in .

Further, the WRF-Hydro model iteration comparison with the time series has been shown in . represents discharges simulated by WRF-Hydro based on the best parameters selected by the DDS algorithm. shows three Events over three years (from 2015 to 2017). In each event, the comparison was made between the true discharge value and the model outputs (Model-A, Model-B, and Model-C). Model-A represents the discharge time series based on the optimal calibrated parameter targeting the discharge Qg (true discharge). Model-B represents the discharge time series based on the optimal calibrated parameter targeting the discharge Qgt (which is a temporally sampled sub-set of Qg). And, Model-C represents the discharge time series based on the optimal calibrated parameter targeting the discharge Qs (same as Qgt but associated with discharge uncertainty). Since the SWOT mission was designed for three years, the WRF-Hydro model calibration was evaluated from 2015 to 2017. The intercomparison of different discharges during extreme events each year is shown in . The intercomparison of different discharges was carried out during the peak flows. It was observed from that for all three events, Model-A, Model-B, and Model-C have captured the streamflow dynamics. For Event-1, Model-A, Model-B, and Model-C were able to capture the streamflow dynamics but with consistent lag. The potential reason for having the consistent lag may be due to MannN parameter values for all the models. Also, the increase in runoff infiltration affects the occurrence of the peak. In the previous studies, Liu et al. (Citation2021) and Dubey et al. (Citation2021), It has been shown that when the value of REFKDT is increased by 0.5, the peak time is delayed by approximately two hours. In the current study, the REFKDT value was ranging from 0.5 to 1.5, with an increment factor of 0.5. Hence, a time lag has been observed. The MannN parameter may have a significant impact on the transit time of the streamflow. The lower the value of MannN, the faster the transit time and, as a result, the higher discharge. It should also be noted that the MannN parameter collaborates closely with REFKDT to influence the simulated hydrograph. Another potential reason for the time lag could be the outflow from the Tawa dam. The Tawa dam, which is in the study domain, covers 3600 grid points. But the reservoir was not modeled in this study due to the unavailability of outflow data from the reservoir. So, the unmodelled reservoir outflow in the channel routing shows the time lag. So, during Event-1 (), in which the maximum flow reaches up to 3000 m3/s, Model-A, Model-B, and Model-C have overestimated the discharge with respect to Qg. However, during the Event 2 (), the peak flow was up to 10000 m3/s. The Model-A, Model-B, and Model-C were able to capture high flow dynamics quite accurately but again overestimated the Eevent-3 when the peak went down to 1500 m3/s. The potential reason for capturing the high peaks by the model would be the objective function KGE, for which the model calibration has been optimized. So, it can be stated that all the models perform well during the high flow or monsoon season compared to low flow. Further, the WRF-Hydro model calibration based on Model-B has similar results as Model-A and Model-C. So, it has been observed that the performance of all models is different for different even though the underlying data used (i.e. a subset from the in-situ discharge data) remains the same.

Figure 4. Calibration of discharge with optimized Model-A, Model-B, and Model-C parameters for the (a) Event -1, (b) Event-2, and (c) Event-3 at Hoshangabad gauge station.

Figure 4. Calibration of discharge with optimized Model-A, Model-B, and Model-C parameters for the (a) Event -1, (b) Event-2, and (c) Event-3 at Hoshangabad gauge station.

In the case of TS alone, shows that taking the area under the curve between ± 20% denotes that more than 90% of iterations have less than 20% absolute difference between Qg and Qgt (similar to Nickles et al. (Citation2020). However, after combining the effect of TS with associated uncertainty, 60% of iteration shows less than 20% absolute difference between Qg and Qs. Furthermore, the density curve is skewed toward the right and has the most percentage difference toward positive values for Qg-Qgt and Qg-Qs. The density curve’s skewness indicates that comparing the Qw with Qg and Qgt gives more positive KGE than Qs. Since the Qgt is derived from Qg and has no uncertainty, It is expected to have more positive KGE in the case of Qg-Qgt compared to Qg-Qs.

Figure 5. Density curve of the percentage difference between time series Qg-Qgt and Qg-Qs. The density curve having an area equal to one represents the effect of SWOT TS alone (Qg-Qgt) and when combined with the uncertainty associated (Qg-Qs) over the KGE values in each iteration. The outlier has not been shown.

Figure 5. Density curve of the percentage difference between time series Qg-Qgt and Qg-Qs. The density curve having an area equal to one represents the effect of SWOT TS alone (Qg-Qgt) and when combined with the uncertainty associated (Qg-Qs) over the KGE values in each iteration. The outlier has not been shown.

Based on the highest KGE values, the best parameter iterations were selected, and it was observed that the Qgt more often performed well with Qg than Qw. To understand the difference in the performance of KGE values for Qgt vs. Qw and Qg vs. Qw, it is important to understand the formation of different discharge time series under comparison. Hence, the daily discharge time series have been considered while comparing Qg vs. Qw. However, the infrequent temporally sampled discharge has been considered in comparing Qgt vs. Qw. Since the model output matches well with the in-situ observed discharge values during the low flow and peak events (), it is admissible that Qgt vs. Qw would provide better KGE values compared to KGE values obtained from Qg vs. Qw. Since the model calibration based on Qg produces more robust model parameters, the improvement in KGE values alone from Qgt does not necessarily represent the model performance (Nickles et al. Citation2020). Hence, it was observed that the Qgt gives better KGE values and represents the monthly peak flow values even though only infrequent temporally sampled SWOT-based discharge has been selected. Contrarily, the Qs were shown lower KGE values due to the combined effect of infrequent TS and uncertainty with a Gaussian error, which indicates a negative bias with a significant deviation or spread.

Figure 6. Histogram of the percentage difference between Qg and monthly mean flow (MMF) i.e. (a) Qg-Model A, (b) Qg-Model B, (c) Qg-Model C and monthly peak flow i.e. (d) Qg-Model A, (e) Qg-Model B, (f) Qg-Model C for 2015-2017.

Figure 6. Histogram of the percentage difference between Qg and monthly mean flow (MMF) i.e. (a) Qg-Model A, (b) Qg-Model B, (c) Qg-Model C and monthly peak flow i.e. (d) Qg-Model A, (e) Qg-Model B, (f) Qg-Model C for 2015-2017.

The Tawa Dam has influenced the natural water flow in the Narmada river basin, which further affects the hydrological model calibration. The WRF-Hydro hydrological model considers the dam as a natural lake and compensates for the flow mainly due to the dam’s unavailability of flow regulation data. Furthermore, the reservoirs may also affect the river’s flow due to significant evaporation loss, which further affects the calibration. However, irrespective of the hydrological model used, we have focused on the influence of infrequent SWOT-based discharge in the calibration parameters in this study. Also, the hydrological model performance may differ with different models and atmospheric forcing, and the current study is based on the calibration uncertainty in using different time series among Qg, Qgt, and Qs.

4. Conclusions

The WRF-Hydro model calibration using discharge derived from the infrequent TS of SWOT has not been significantly different from daily in-situ discharge. Moreover, the SWOT-based discharge sometimes performed well than the daily in-situ discharge. On analyzing the DDS calibration iterations, it has been observed that the more than 90% of parameter iterations have KGE values with less than 20% absolute percent difference when only SWOT TS alone has been considered. Furthermore, the monthly mean and maximum flow values at the Hoshangabad gauge station have an average percentage difference of less than 10% for the best parameter iteration. These minor differences suggest that the WRF-Hydro hydrological model performance does not vary much by either calibrating using SWOT-based discharge or daily in-situ discharge. Even though the SWOT has infrequent TS and likely uncertainty, the SWOT-discharge-based calibrated hydrological model performed well in capturing the peaks and low values of discharge. This study suggests that the SWOT-based discharge helps calibrate the hydrological model when no in-situ flow information is available. This study will help downstream stakeholders to understand and monitor the catchment using hydrological modeling and SWOT data when upstream flow regulation information is limited. The results of the current study may vary with the use of the different hydrological models and atmospheric forcing data. However, further study is needed to investigate flood event forecasting based on calibration using infrequent temporally sampled SWOT discharge data.

Acknowledgements

Authors thank the support through DST CNRS project (DSTCNRS/2018-19-01/109) and the support through DST Centre of Excellence in Climate Studies, IIT Bombay through project DST/CCP/CoE/140/2018(G).

Disclosure statement

No potential conflict of interest was reported by the authors.

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