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Article

Incorporating Weather Attribution to Future Water Budget Projections

Southwest Research Institute, San Antonio, TX 78238, USA
Hydrology 2023, 10(12), 219; https://doi.org/10.3390/hydrology10120219
Submission received: 10 October 2023 / Revised: 7 November 2023 / Accepted: 18 November 2023 / Published: 22 November 2023

Abstract

:
Weather attribution is a scientific study that estimates the relative likelihood of an observed weather event occurring under different climate regimes. Water budget models are widely used tools that can estimate future water resource management and conservation conditions using daily weather forcing. A stochastic weather generator (WG) is a statistical model of daily weather sequences designed to simulate or represent a climate description. A WG provides a means to generate stochastic, future weather forcing to drive a water budget model to produce future water resource projections. Observed drought magnitude and human-induced climate change likelihood from a weather attribution study provide targets for WG calibration. The attribution-constrained WG approximately reproduces the five-fold increase in probability attributed to observed drought magnitude under climate change. A future (2031–2060) climate description produced by the calibrated WG is significantly hotter, with lower expected soil moisture than the future description obtained from global climate model (GCM) simulation results. The attribution-constrained WG describes future conditions where historical extreme and severe droughts are significantly more likely to occur.

1. Introduction

Weather attribution is the determination of the relative likelihood or probability of a weather event occurring under two different climate descriptions. It has been used to analyze changes in likelihood, relative to undisturbed early 20th century conditions, for an observed drought or precipitation event under present-day human-induced climate change conditions [1]. A specific drought or storm event is an example of weather, which comprises daily atmospheric events. Weather describes short-term atmospheric events that occur over minutes to weeks [2]. Climate describes the weather of a place averaged over an interval of a couple of decades or longer [3].
Water budget or balance models are widely used in hydrology and water resources applications. They have been implemented to estimate a range of water resources considerations, including irrigation demand, soil moisture stresses, predicting stream flows, and assessing the hydrologic effects of climate change and changes in vegetation cover [4,5]. Water budget models generally utilize hourly to monthly weather forcing as the external driving force in their calculations [4,5,6,7].
Observations of future weather are unavailable. When future water budget projections are made using a water balance model, future weather is provided as input forcing. Stochastic or random realizations of future weather sampled from a physical process-based climate representation can provide future weather forcing to a water balance model. A collection of sampled realizations from a climate scenario representation is an ensemble. Global climate model (GCM) simulation results have been used to generate future weather ensembles for input to water balance models. GCMs are coupled atmosphere–ocean, general circulation models that simulate global weather with a sub-daily time step. GCMs simulate stochastic future weather to generate a physics- and process-based description of future climate [7,8].
Another option for the creation of stochastic realizations of future weather is a stochastic weather generator (WG) [7,8]. A WG is a statistical model of daily weather sequences that is designed to simulate or represent key statistical properties of observed meteorological records, like means, variances, frequencies, and extreme occurrences. When used in Monte Carlo simulations to generate many stochastic realizations of day-to-day weather, a WG is essentially a random number generator whose time-aggregated outputs statistically describe climate [9].
WGs that statistically reproduce a future climate description obtained from GCM simulation results have been previously used to attribute hydrologic changes to global climate change, e.g., Refs. [7,8,10,11,12,13,14,15]. This study employs the unique approach of calibrating or training a WG to reproduce drought likelihood and drought magnitude from an attribution study. The calibrated WG provides a means to incorporate weather attribution into future water budget projections. The attribution-constrained future climate is compared to the projected climate from GCM simulation results and the historically observed climate. It indicates an increased likelihood for droughts of historically severe magnitudes relative to those projected by GCM simulations.

2. Data and Methods

A study area, discussed in Section 2.1, is used to facilitate the acquisition of observed weather and future projected climate on the watershed scale. Observed weather for the site is discussed in Section 2.2, and a future climate description is presented in Section 2.3.
An attribution study combined with drought index calculations constrains WG formulation. Weather attribution is discussed in Section 2.4, two drought indexes are presented in Section 2.5, and WG formulation is described in Section 2.6 and Section 2.7. Finally, automated calibration implementation is discussed in Section 2.8.

2.1. Study Site

The study area was the Frio River basin in south-central Texas (TX), which is shown in Figure 1. This basin is about 134 km west of San Antonio, TX. The Frio basin is important from a water budgeting perspective because the Frio and Dry Frio Rivers cross the Balcones Fault Zone (BFZ) Edwards Aquifer Recharge Zone within the watershed. In the Recharge Zone, direct communication between surface water and subsurface storage is feasible and likely to occur due to the karstic nature of the Edwards Aquifer.

2.2. Weather Observations

Daily precipitation depth, maximum temperature, and minimum temperature observations were acquired for the study area, see Figure 1, for 1 January 1980 through 31 December 2022 from the Daymet version 4 repository [16,17]. Daymet provides long-term, continuous, gridded estimates of daily weather and climatology variables by interpolating and extrapolating ground-based observations through statistical modeling techniques [16].
These datasets are available on a 1 km × 1 km spatial grid, which is displayed in Figure 1. Gridded estimates of daily weather are regionalized to provide a time series of daily weather parameters for the Frio basin. This regionalization is implemented using proportional area weighting, where grid cell values are weighted by the ratio of the grid cell area within the Frio basin to the entire area of the Frio basin. Monthly-averaged temperature and precipitation during 1991–2020 are presented in Figure 2.

2.3. Future Climate Projections

The Coupled Model Intercomparison Project (CMIP) is a foundational element of climate science because it coordinates the design and distribution of GCM simulations of the past, current, and future climate [18]. The most recent ensemble of CMIP-endorsed model intercomparison projects is Phase 6 or CMIP6. It contains 23 endorsed or approved GCMs [19].
Each CMIP6 model may be used to simulate one or more scenarios, as defined in the CMIP6 experimental design. In this study, the shared socioeconomic pathway (SSP) 5 with a 2100 radiative forcing level of 8.5 watts per square meter (W/m2) is the only CMIP6 scenario examined; this scenario is commonly labeled as ssp585. SSP5 represents a development path that is fossil-fueled and carbon emissions-intensive. It is predicated on the assumption of increasing integrated global markets, leading to innovations and technological progress. The social and economic development in this scenario is based on intensified exploitation of fossil fuel resources, characterized by a high percentage of coal usage and an energy-intensive lifestyle worldwide [20,21].
CMIP6 provides a collection of 23 global-scale climate simulation models. For application to a relatively small region like the Frio basin, as seen in Figure 1, the CMIP6 results need to be downscaled or interpolated to a more refined grid. CMIP6 results for the ssp585 scenario that were downscaled using the Localized Constructed Analogs version 2 (LOCA2) approach [22,23,24,25] were used for future climate projections. The LOCA2 grid configuration is shown in Figure 1.
LOCA2 statistical downscaling uses a 6-km resolution. The primary improvement of LOCA2, compared to the earlier version of LOCA, is in the representation of precipitation extremes [22,23]. LOCA2 downscaled CMIP6 ssp585 simulation results were obtained for daily maximum air temperature, daily minimum air temperature, and daily precipitation depth for the period from 1 January 2021 through 31 Decemebr 2065. The LOCA2 CMIP6 ssp585 results were regionalized to provide a unified time series of daily weather parameters for the Frio basin from each of the 23 CMIP6 models. This regionalization is implemented using proportional area weighting, where grid cell values are weighted by the ratio of the grid cell area within the Frio basin to the entire Frio basin area. Hereafter, “LOCA2” will refer to the ensemble of LOCA2 downscaled results from the 23 CMIP6 models for emissions scenario ssp585.
LOCA2 projected future climate is compared to the historically observed climate in Figure 2, Figure 3 and Figure 4. Figure 2 and Figure 3 show that temperature is expected to consistently increase in the future. Figure 2 and Figure 4 suggest that annual and seasonal precipitation depths will be similar, but decline slightly, for future conditions, relative to the historical observations.

2.4. Weather Attribution

Event attribution studies calculate if—and to what degree—a specific extreme event is made more likely or intense by climate change [1]. World Weather Attribution (WWA) refers to a collaboration of scientists from various organizations that have conducted numerous human-induced climate change attribution studies since the 2000s. The goal of WWA is to produce scientifically defensible attributions on short time scales following events with large impacts. WWA’s experience in attribution studies has led to the development of an eight-step procedure [26]: (1) analysis trigger, (2) event definition, (3) observational trend analysis, (4) climate model evaluation, (5) climate model analysis, (6) hazard synthesis, (7) analysis of trends in vulnerability and exposure, and (8) communication.
A detailed discussion of event attribution procedures is provided in Ref. [27]. Typically, the result of an attribution study takes the form of a probability ratio (PR). The PR is generally expressed as “the event has become X times more/less likely due to climate change with a 95% confidence interval of Y to Z”. The PR is often combined with an intensity impact summary, such as “the heat wave has become T (T1 to T2) degrees warmer due to climate change [26]”.

2.4.1. Summer 2022 Attribution Study

North America experienced an unusually warm summer in 2022, compared to prior observations, accompanied by abnormally dry soil conditions. High temperatures lead to increased land evapotranspiration and are, consequently, the main drivers of dry soil conditions. The WWA conducted an attribution study for the combined drought and heat wave in the summer of 2022. For the Northern Hemisphere extratropics, i.e., the region between the Tropic of Cancer (23.5° north of the equator) and the Arctic Circle (66.5° north of the equator), human-induced climate change made the observed soil moisture drought in June, July, and August of 2022 at least five times more likely for surface soil moisture, relative to the null hypothesis of no human-induced climate change [28].
To determine that the observed summer of 2022 surface soil moisture deficit was five times more likely to occur under human-induced climate change, Ref. [28] used three multi-model ensembles from different climate modeling experiments. One ensemble came from CMIP6, which used historical simulations from 1850 to 2015 compared to the ssp585 scenario for the 2016–2099 period. The second ensemble included the AM2.5C360 and FLOR high-resolution climate models developed at the Geophysical Fluid Dynamics Laboratory (GFDL). The HighResMIP SST-forced model ensemble, where SST stands for sea surface temperature, provided the third ensemble.

2.5. Drought Indexes

Drought is defined as “a deficiency of precipitation over an extended period of time (usually a season or more), resulting in a water shortage [29]”. Different types of droughts are sometimes labeled as meteorological and hydrological droughts. Meteorological drought refers to a period of extended precipitation deficiency. Hydrological drought refers to a period of extended low water supply [29].
Overallocation of resources to agricultural, domestic, and industrial consumption is at least as significant as precipitation deficiency in creating extended periods of low water supply. Overallocation is a widespread issue, often resulting from a combination of overly optimistic assessments of expected water resources and gross resource mismanagement [30,31]. This study focuses on weather and climate parameters, employing the standard definition of drought as an extended period of precipitation deficiency.
Drought indices are commonly used as probabilistic, statistical tools to identify drought severity and guide resource conservation and management. The probabilistic component of these indices is important because it allows for their use in risk and decision analysis [32]. Two different drought indexes are used: (1) standardized precipitation index (SPI) and (2) standardized precipitation evapotranspiration index (SPEI).

2.5.1. Standardized Precipitation Index (SPI)

SPI was developed to provide a better representation of abnormal wetness and dryness than previous indices. It is computed from a precipitation total over a pre-selected duration, like 3, 6, or 12 months [33,34]. The SPI is a probability-based index, designed to be a spatially invariant indicator of drought that acknowledges the importance of time scales in analyzing water availability and use. Essentially, it is a standardizing transform of the probability of observed precipitation [32], which is equivalent to the power transform algorithm used for the standardization of features and outcomes in machine learning [35].
The probabilistic component of the SPI involves fitting a probability distribution to collections of cumulative monthly precipitation totals for each year in a dataset. An SPI value is calculated for each month in the underlying precipitation dataset. Because the SPI is derived from a collection of annual values, it provides an intrinsic return period calculation. Table 1 presents SPI drought intensity definitions. Negative SPI values denote precipitation deficiency, i.e., drought, and positive SPI values denote precipitation excess. The sum of SPI values over consecutive months can be used as a drought magnitude index to compare different periods of historical drought periods [34].
Figure 5 graphically demonstrates the standardizing transform that constitutes the SPI calculation. This figure shows the fitted distribution type for the SPEI; however, the SPI transform is identical to the SPEI transform. The SPEI uses deficit and a log-logistic distribution while the SPI uses precipitation and a gamma distribution. It should be noted that the implementation of the SPI in this work follows the approach of using the gamma distribution as per Refs. [33,34], rather than the Pearson type III distribution recommended by Ref. [32].
The calculation of the SPI is subject to the “problem of zeros”, where it is possible for the cumulative precipitation across 3- and 6-month intervals in the study area to be zero. This results in an undefined return period due to a cumulative probability, F, as shown in Figure 5, of zero. Cumulative precipitation must be greater than zero for the return period estimation. To address this issue, a minimum F value of 0.16667 = 1.0 / ( 2 × 30 ) is enforced. A gamma distribution is fit to the annual values across 1981–2010, which is 30 years. N denotes the number of years, and the minimum F value respects the 2 × N maximum recurrence interval rule-of-thumb as outlined in Ref. [36].

2.5.2. Standardized Precipitation Evapotranspiration Index (SPEI)

The SPEI was developed to provide a climatic drought index that is sensitive to global warming. It is based on precipitation and temperature data, thus incorporating sensitivity to temperature increases and global warming considerations. The SPEI has the advantage of combining multiple parameters, providing the ability to include the effects of temperature variability on drought assessment [37].
The SPEI is congruent with the SPI, with the primary difference being the use of monthly water deficit (D) values in place of monthly precipitation (P) values. Equation (1) presents the definition of D where P E T denotes potential evapotranspiration. P E T in this study is calculated using the approach described in Appendix A.2.
The purpose of including P E T in the drought index calculation is to obtain a relative estimation of time-varying dryness potential; consequently, the method used to calculate P E T is not critical to SPEI implementation. “Temperature-only” P E T estimates are generally used to provide a direct tie to global warming projections [37]. A positive D value denotes a monthly water surplus, and a negative D value identifies a monthly water deficit.
D = P P E T
Figure 5 provides a graphical description of the SPEI standardizing transform. Note that because the SPEI is a Z-score transform, just like the SPI, the drought intensity definitions in Table 1 also apply to the SPEI.

2.6. Using Drought Indexes with Weather Attribution

The standardizing transform integral to drought index determination assigns a probability value to each cumulative D for SPEI or cumulative P for SPI. Ref. [28] conducted a human-induced climate change attribution study for North America focusing on the drought during the summer of 2022. The study found that climate change made the observed soil moisture drought five times more likely, as discussed in Section 2.4.1. This attribution study, in conjunction with the SPEI calculated using the 1981–2010 Climate Normals, is used to establish targets for weather generator calibration through the following steps
1.
Log-logistic distribution fit to 3-month cumulative D values from 1981–2010.
  • 1981–2010 is within the historical period of 1850–2015 used in the attribution study.
2.
Observed 3-month cumulative D transformed to SPEI using Figure 5 for 1993–2022 and the log-logistic distributions fit to the 1981–2010 observed values.
  • The lowest SPEI identified from July and August 2022 has the target drought magnitude, and July 2022 for the Frio basin has the lowest SPEI.
3.
The observed 3-month cumulative D for July 2022 SPEI provides the drought magnitude.
  • Historical probability, F, of the July 2022 drought magnitude is determined as part of the SPEI calculation in item no. 2.
4.
Historical July 2022 likelihood, F, is multiplied by 5 to obtain the target, human-induced climate change probability for the July 2022, 3-month cumulative D.
  • The July 2022, 3-month cumulative, D, denotes the observed drought magnitude.
  • 5 × F denotes the “new” likelihood of the observed drought magnitude under human-induced climate change conditions.

2.7. Weather Generators (WGs)

A WG is a stochastic, statistical model of daily weather sequences. When a weather generator reproduces key statistical properties of meteorological records, it provides a concise distillation of the climate. WGs are commonly used in water resource planning and design, and agricultural, ecosystem, or climate change analysis applications because meteorological data may lack temporal or spatial coverage for the area of interest. WGs are not weather forecasting algorithms or deterministic weather models; consequently, it is not expected that a stochastically simulated weather sequence will be duplicated exactly by historical or future weather observations [9]. In the same way, it is not expected that weather sequences observed in the future will exactly duplicate historically observed weather sequences because the atmosphere provides an inherently chaotic system.
Daily precipitation depth, maximum air temperature, and minimum air temperature are stochastically simulated using a weather generator in this study. The simulation of precipitation depth includes the depiction of precipitation occurrence and intensity. Occurrence is represented by two states: (1) wet and (2) dry. In the dry state, precipitation depth is always zero. In the wet state, intensity, or daily precipitation depth, is stochastically simulated. Air temperature simulation is conditional upon the current state. Figure 6 provides a schematic showing weather generator formulation and operation.

2.7.1. Precipitation Occurrence with Spell Lengths

Alternating spell lengths are used to represent precipitation occurrence. The duration of a spell length for a state is sampled from a negative binomial distribution for that state. When the spell length duration has elapsed, a duration for the spell length of the other state is sampled from a negative binomial distribution for the new state. Every time a spell length elapses, the process is repeated, toggling to the other state for the selection of a new spell length, creating an alternating renewal process representation [9].
Negative binomial distributions are used to represent the spell-length likelihood and magnitude for both states and each month. This means that precipitation occurrence is represented by 24 (2 states × 12 months = 24) negative binomial distributions. The negative binomial probability distribution represents a discrete random variable. It describes a sequence of independent and identically distributed (i.i.d.) Bernoulli trials, repeated until a predefined, non-random number of successes occurs [38].
The negative binomial discrete random variable object from the SciPy stats library [38] is used in this study. It is defined using two shape parameters, N and P, and a location specification. N denotes the number of successes, and P denotes the probability of a single success [38]. N and P are the parameters for each of the 24 negative binomial distributions that are determined through calibration. The location parameter is set by the state. For wet-state distributions, a location parameter value of one is used, and a location parameter value of two is used for dry-state distributions.

2.7.2. Precipitation Intensity

The two-parameter gamma distribution provides precipitation intensity representation. A unique gamma distribution is used for each month, providing a total of 12 gamma distributions within the WG. The two-parameter gamma distribution is commonly used to represent precipitation intensity in weather generators [9].
A generalized form of the gamma probability distribution for a continuous random variable from the SciPy stats library [38] is used in this study. The generalized form accepts a location and scale parameter in addition to the two shape parameters, a and c. The scale, a, and c are the three parameters determined through calibration. The location is set to 0.255 mm for all gamma distributions and specifies the minimum precipitation intensity (0.255 mm/day) that can be simulated.
A truncation threshold is also used for each month to cap the maximum allowable daily precipitation depth estimated by the WG. This threshold is set to the 95th percentile daily precipitation depth observed for the month from 1991 to 2020.

2.7.3. Air Temperature

Other weather parameters, besides precipitation depth, have been simulated in WGs. Examples include temperature, solar radiation, and wind speed [39,40]. Here, the maximum and minimum daily temperatures are non-precipitation parameters.
The representation of maximum and minimum daily temperature is conditioned upon the precipitation state. Conditioning temperature on the presence or absence of precipitation serves as a simplistic proxy for unrepresented processes like cloud cover [41].
Air temperature is conditioned on the precipitation state and calculated during stochastic simulation using methods from the WGEN weather generator [39,40,42]. This approach for non-precipitation variables is based on a first-order vector autoregression, which requires that the statistics of the current day’s values are fully determined by the values on the previous day [9]. The conditional calculation for air temperature is presented in Appendix A.3.
One modification to the state-conditional temperature calculation described in Appendix A.3 is the inclusion of an additive scalar, C, for daily minimum and maximum air temperatures and for each state, as shown in Equation (2). The additive scalar term provides a simple means to uniformly increase stochastically simulated temperatures, and it is determined through calibration.
T k t = μ k , 0 t + C k , 0 + σ k , 0 t z k t if day is dry μ k , 1 t + C k , 1 + σ k , 1 t z k t if day is wet
In Equation (2), subscript k denotes the index number that identifies non-precipitation weather variables. It ranges from 0 to 1, where 0 represents the daily maximum air temperature, and 1 represents the daily minimum air temperature. Subscript 0 in “ k , 0 ” signifies the dry state and 1 in “ k , 1 ” signifies the wet state. μ and σ in Equation (2) denote the mean and standard deviations, respectively. z denotes Z-scaled or normalized residual elements that provide white noise-type adjustments to calculated temperature values. Finally, t identifies the Julian daytime index, which goes from 1 to 365 for “standard” years and 1 to 366 for leap years.

2.7.4. Extreme Precipitation Events

Extreme precipitation events are expected to become more intense as average temperatures increase. Additionally, consistent temperature increases are expected to produce more frequent drought conditions [43]. An extreme event representation was included within the WG to statistically represent the contrasting impacts of consistent warming: (1) more intense and frequent droughts combined with (2) more intense extreme precipitation events.
Extreme events are included in the WG, as shown schematically in Figure 6. When an event is triggered, the event magnitude overwrites the next wet day precipitation depth. This formulation allows wet spell length distributions, see Section 2.7.1, and wet day precipitation depth distributions, see Section 2.7.2, to portray the expectation for more intense droughts while including more intense extreme precipitation through the extreme precipitation event representation.
An event formulation includes the timing and magnitude of the event. Event objects follow Poisson distributions for interarrival times, enabling a stochastic representation of the occurrence time. They also employ uniform distributions for event magnitude. The Poisson distribution for interarrival times is parameterized using the mean recurrence interval in years for the event. The uniform distribution, which determines event magnitude, is parameterized with lower and upper magnitude bounds. The lower boundary is set at the current estimated event depth for the basin centroid for the average recurrence interval, as per Ref. [44], which is NOAA Atlas 14. The upper boundary magnitude is a calibration parameter. Table 2 outlines the extreme event configuration for calibration, along with 24-h point precipitation depth estimates from Ref. [44].

2.8. Calibration

The automated calibration or training was implemented with PEST, which stands for “parameter estimation” [45,46]. Parameter estimation with PEST employs an inverse-style approach where model parameters are estimated by varying parameter values to find values that produce the “best-fit” between simulated values and target observations. PEST provides data assimilation (DA) that seeks to combine information from model simulations with observations to obtain the “best” description of a system along with an accompanying description of uncertainty. Consequently, PEST really provides “calibration-constrained uncertainty analysis” rather than just “parameter estimation” [45].
The parameters, for which PEST seeks optimal values in this study, are mostly definition parameters for the probability distributions that comprise the WG, as discussed in Section 2.7. Appendix A.4 provides calibration parameters along with the ranges of values examined. Target observations are derived from the SPEI and weather attribution analyses; they are discussed in Section 3.1 and summarized in Appendix A.4.

3. Results

A weather attribution study is used to develop the target outcomes for WG training. A WG is then calibrated to simulate the best-fit outcomes and applied to produce weather attribution-guided future climate projections for the Frio basin.

3.1. Drought Targets from Weather Attribution

Target drought magnitude and likelihood, given human-induced climate change, are developed according to the procedures outlined in Section 2.6. The observed 3-month cumulative D for July 2022 is 540 mm, which serves as the target drought magnitude for July. A historical SPEI of 1.9 for July 2022, with an associated cumulative probability, F, of 0.030 , is determined using a log-logistic distribution. This distribution is fit to the collection of 30 observed July 3-month cumulative D values from 1981 to 2010.
As noted in Section 2.6, July 2022 provides the lowest SPEI and 3-month cumulative D from the June, July, and August 2022 periods examined in the attribution study. Table 3 SPEI- and SPI-related values from May to September 2022. There was some precipitation, P, in August 2022, as indicated by the August 2022 3-month P and SPI values, which broke the severe drought earlier in this localized region than what was experienced across the majority of the Northern Hemisphere extratropics.
The target likelihood for the observed July magnitude of 540 mm is five times the historical likelihood [28], or 5 × 0.030 = 0.149 . This drought likelihood analysis under human-induced climate change is extended to the other calendar months by extracting the 3-month cumulative D for each month corresponding to a cumulative probability of F = 0.030 . The extracted, cumulative D denotes the drought magnitude target for each month. The corresponding cumulative probability target for each month is then F = 5 × 0.030 = 0.149 . Table 4 provides the drought magnitude and likelihood targets for each month.

3.2. Weather Generator Calibration

The purpose of calibration is parameter estimation. Optimal parameter values are those that produce the closest match between simulated values and target observations. Parameters, which are varied as part of calibration, are listed in Table A1, Table A2, Table A3, Table A4 and Table A5, along with the “optimal” or final parameter values. Target observations are described in Table A6. Best-fit simulated target values are provided in Table A6 and Table 4.
The annual average precipitation depth, P, was used as a target observation in addition to the monthly drought likelihood and magnitude values. Simulated annual average climate parameters from 2031 to 2060—from the calibrated WG—are compared to the historical observations from 1991 to 2020 and LOCA2 projected values from 2031 to 2060, as seen in Table 5.

3.3. Attribution-Constrained Future Climate Projections

The calibrated WG was used to make future climate projections from 1 January 2024 to 31 December 2065. A total of 1000 stochastic realizations of daily weather are used to generate the future climate description. The weather generator (WG) 2031–2060 future climate description is compared to the LOCA2 2031–2060 future climate description and the observed 1991–2020 climate description. Table 5 provides a comparison of the annual average P, P E T , and D.
Figure 7 compares the monthly-average P, monthly-average daily maximum temperature, and monthly-average daily minimum temperature among WG 2031–2060 projected values, LOCA2 2031–2060 projected values, and 1991–2020 observed values. The attribution-constrained WG produces consistently warmer daily maximum temperatures and consistently cooler daily minimum temperatures than the LOCA2 2031–2060 values.
Figure 8 presents the WG-projected annual average temperature cone of uncertainty. In this case, the cone of uncertainty is flat because the WG formulation is stationary in time. Figure 9 displays the WG-projected annual precipitation depth cone of uncertainty. The distribution of annual precipitation depth is compared in Figure 10 among WG 2031–2060 projected values, LOCA2 2031–2060 projected values, and 1991–2020 observed values. The WG 2031–2060 mean annual P is approximately equal to the observed 1991–2020 mean annual P. LOCA2 projects a smaller mean annual P than the other two datasets.

Drought Conditions

The WG is calibrated or trained to portray a drought magnitude, which has a recurrence interval of approximately 33 years ( 33.3 = 1.0 / 0.030 ) under historical 1981–2010 conditions, with a recurrence interval of approximately seven years ( 6.7 = 1.0 / 0.149 ) for future projected conditions. The cumulative 3-month D is used to define a drought magnitude, as shown in Table 4.
The observed 3-month D from 1993 to 2022 is used in Figure 11 to compare the relative drought conditions among the observed 1981–2010, LOCA2 projected 2031–2060, and WG-projected 2031–2060 conditions. When 1993–2022 observations are analyzed from the perspective of the WG 2031–2060 climate, there are no severe drought periods during the 1993–2022 period. A severe drought has an SPEI of 1.5 from Table 1. Figure 11 demonstrates that the WG 2031–2060 climate is significantly warmer and drier than the LOCA2 2031–2060 climate and the observed 1981–2010 climate.
The observed P from 1993 to 2022 is used in Figure 12 to compare SPI-derived relative drought and wetness conditions among the observed 1981–2010, LOCA2 projected 2031–2060, and WG-projected 2031–2060 conditions. SPI depends only on P. Figure 10 shows that the annual average P values are approximately equal for the WG-projected 2031–2060 and observed 1991–2020 conditions and that the annual average P is expected to be smaller for the LOCA2 projected 2031–2060 conditions. Additionally, the WG-projected 2031–2060 conditions have the most large and small outliers, denoting an increased expectation for extreme events while maintaining a constant annual average P from the observed 1991–2020 conditions. Comparative results in Figure 12 agree with the comparisons among WG, LOCA2, and observed conditions in Figure 7 and Figure 10.

4. Discussion

CMIP6 simulations offer stochastic, day-to-day weather that is derived from a robust physical representation of future climate, based on idealized initial conditions and forcing scenarios. CMIP6 models represent the physics and physical processes in the atmospheric system. From the viewpoint of stochastic simulation, CMIP6 results provide stochastic day-to-day weather, sampled from the governing or underlying “climate” process, as well as a physics-based description of the “climate” process and its functions under varying initial and forcing conditions.
Stochastic WGs produce stochastic day-to-day weather, which is sampled from an underlying stochastic “climate” process that is specified when the WG is formulated. The underlying “climate” process is primarily specified through configuration and parameterization of the probability distributions that comprise the WG, as shown in Figure 6. For WG, the underlying “climate” process is external to the WG and must be derived or depicted based on other sources of information.
CMIP models are clearly superior to WGs in many cases because they provide stochastic day-to-day weather sampled from the underlying “climate” process and the physics-based description and representation of the “climate” process. A WG can only provide stochastic day-to-day weather sampled from an externally specified “climate” process. One scenario for which WGs provide additional utility relative to CMIP models is the case where the “climate” process has been described from other sources and datasets and is different in some manner from the “climate” process representation provided by CMIP models. An example of this scenario is the representation of extreme events.
Extreme events fall within the tails of the long-term aggregated description of weather that constitutes climate. A climate description can provide a probability for the occurrence of a generic event magnitude. However, for analyzing the likelihood of a regional-scale event, CMIP models alone are insufficient, as they are global in scale. In such analyses, CMIP simulation results are often augmented with other information sources, such as high-resolution, regional geophysical models and sea surface temperature models.
An observed event is weather, not climate. Weather attribution is a formalized and scientific approach used to identify the change in likelihood or PR for an observed event under two different climate regimes. Attribution provides the “new” or future probability of occurrence for event magnitude. Weather attribution is used in this study to generate drought magnitude and likelihood targets for WG calibration, and attribution provides the “climate” process description that is different from that contained within CMIP results.
Two advantages to using WGs are: (1) WGs can represent a “climate” process that is different from that represented in CMIP results and (2) WGs can easily produce large numbers of stochastic realizations, i.e., tens to hundreds of thousands. A large number of realizations is required to ensure robust sampling of the stochastic weather forcing input variables to a water balance model for every model input time in a water balance model. If biased forcing, resulting from the use of too few realizations, is propagated through a water balance model, then the resulting water budget estimates will also be biased.
As an example of the importance of robust sampling, the 95th percentile time history in Figure 4 shows a peak of about 1750 mm in 2030. This is not a future prediction contained within the LOCA2 results for the increased likelihood of a very wet year in 2030. The occurrence of a wet year in 2030 is a weather event and is only evident in Figure 4 because 23 stochastic realizations of day-to-day weather are employed to generate the figure.
A climate description used for the forcing of a water budget model should provide approximately the same likelihood for an annual precipitation depth value for every year between 2030 and 2040. In Figure 9, the 95th percentile time history ranges between 1048 and 1102 mm between 2030 and 2040. A total of 1000 stochastic realizations were used to produce Figure 9; the 95th percentile time history is not as flat as would be necessary to indicate the same likelihood for an annual precipitation depth of about 1075 mm for each year between 2030 and 2040. As the number of stochastic realizations of day-to-day weather increases, probabilistic time histories, such as the 95th percentile, will become flatter within an interval of assumed stationarity.
Time stationarity is the assumption that time series statistical properties do not change across an interval. Strict stationarity is generally too restrictive, and a reduced requirement, called weak stationarity, is often used. Weak stationarity imposes restrictions on the first two statistical moments of the time series; it formally requires a constant mean and an autocovariance function that depends only on the time difference or lag and is independent of the specific points in time that are differenced [47,48]. The WG formulation presented in Figure 6 enforces strict stationarity across the simulation interval because the probability distributions that comprise the WG are defined in generalized form, requiring three to four parameters, and the parameters that define the probability distributions are held constant across the simulation interval.
Two disadvantages of using WGs relative to CMIP results are: (1) WGs are purely statistical and probabilistic, relying on robust sampling to produce a meaningful climate description, and (2) WGs inherently require the assumption of time stationarity and cannot represent the physics-based evolution of process functions to produce trends. An example of the first shortcoming can be seen in Figure 7, where the structure of the P E T calculation employed in this study pushes the calibrated WG daily maximum and minimum temperatures apart in order to increase the calculated P E T to meet the constraint of the drought targets. The LOCA2 results in Figure 7 suggest a more likely future climate description, where both maximum and minimum temperatures increase uniformly and there is relatively constant increase in the projected future temperature. An example of the second shortcoming is presented in Figure 8, where the calibrated WG simulated annual average temperature is relatively flat or constant across the simulation interval. An improved representation is provided in Figure 3, where there is a trend of an increasing average annual temperature across the analysis interval. One approach that can be implemented with WGs to partially represent trends is to use several intervals of assumed stationarity to reproduce the trend in a step-wise fashion [7,8].
Stochastic simulation is a system simulation that uses variables that can change randomly with individual probabilities for each variable [49,50]. When an ensemble of stochastic realizations of day-to-day weather is used for input water budget model forcing, then the water budget simulation framework is stochastic. When observed weather forcing is used for input water budget model forcing and resulting water budget calculation outputs are compared to observations, like in traditional model calibration, the water budget simulation framework is deterministic. For both types of inputs (stochastic and observed), the water budget model itself, in contrast to the simulation framework, is deterministic if it always produces the same results for the same inputs.
For stochastic simulation, the sampling of variables, which change randomly with individual probability distributions, directly controls the quality of the results obtained. Sampling bias is an error in estimates or simulation results due to a sampling procedure that is not representative of the underlying population described by the probability distribution [51]. In many cases, the sampling of the stochastic inputs is more important than the deterministic water budget model used to propagate uncertainty from stochastic inputs to estimates or outputs.
When stochastic inputs or variables are used and the water budget modeling framework is stochastic, simulation results must be presented probabilistically with cones of uncertainty, similar to what is done in Figure 8 and Figure 9, or as long–term ensemble averages, as done with the Climate Normals in Figure 7. The simulation results for a single outcome realization always present sampling bias because a single outcome realization is derived from a single input forcing sample.

Future Work

WG formulation in this study focuses on reproducing attribution study likelihoods and historically observed annual average precipitation depth. CMIP6 ssp585 simulation results are used in the attribution study to determine the change in likelihood but are not directly employed as targets for WG training.
Future work will examine explicitly combining CMIP simulation results and weather attribution to generate a comprehensive set of targets for WG calibration. Specifically, it would be interesting to use the annual average precipitation depth and 2031–2060 average monthly precipitation depths, see Figure 7, from the LOCA2 2031–2060 climate description, in addition to the drought likelihood and magnitude values, see Table 4, as calibration targets.

5. Conclusions

Weather attribution provides drought magnitude and likelihood targets for WG calibration. Drought conditions of the magnitude observed for the study area during June, July, and August 2022 are expected to be five times more likely to occur under human-induced climate change conditions relative to the historical conditions. A WG is calibrated for the study area to approximately reproduce the five-time increase in probability for historically severe droughts. The 2031–2060 climate description produced by the calibrated WG is significantly hotter and has lower expected soil moisture compared to the 2031–2060 climate description obtained from LOCA2 simulation results.
Projected future day-to-day weather provides stochastic forcing when used to generate water balance model projected outcomes. A WG that is calibrated to reproduce observed weather event magnitude and likelihood for a “new” or different climate regime, such as human-induced climate change relative to pre-industrial conditions, offers an alternative to the climate description provided by GCM simulation results. The attribution-constrained WG future climate description can portray more extreme conditions and events than those obtainable from a global-scale model driven by idealized forcing and initial conditions.

Funding

This research was funded by the Edwards Aquifer Authority (EAA) under contract 23-020L-AMS.

Institutional Review Board Statement

Not applicable.

Data Availability Statement

The weather generator produced data presented in this study are available from the project GitHub per Appendix A.1. The weather generator produced data sets are the only new data created and analyzed in this study.

Acknowledgments

Andrew Kazal from ICF extracted the LOCA2 datasets from public repositories and clipped them to the study area, simplifying the analysis of these datasets. The author wishes to acknowledge the contributions of the four anonymous reviewers whose comments and suggestions improved the quality of this paper.

Conflicts of Interest

The funding sponsors had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, and in the decision to publish the results. The author declares no conflict of interest.

Abbreviations

The following abbreviations are used in this manuscript:
AETactual evapotranspiration
BFZBalcones Fault Zone
CMIPcoupled model intercomparison project
DAdata assimilation
EAAEdwards Aquifer Authority
ETevapotranspiration
GCMglobal climate model
HS85Hargreaves–Samani 1985 equation for E T o
iidindependent and identically distributed
LOCA2localized constructed analogs version 2
PETpotential evapotranspiration
PRprobability ratio
SPEIstandardized precipitation evapotranspiration index
SPIstandardized precipitation index
SSPshared socioeconomic pathway
WGstochastic weather generator
WWAWorld Weather Attribution

Appendix A

Appendix A.1. Source Code Availability

The “New” weather generator source code and associated calibration files are available online from the project GitHub repository at:
https://github.com/nmartin198/wattrib_wg_frio (accessed on 10 October 2023)

Appendix A.2. Potential Evapotranspiration (PET) Calculation

Evapotranspiration (ET) is typically the primary way water is subtracted from a watershed. It includes water loss from the leaves of plants, known as transpiration, and water that evaporates from the soil surface, puddles, ponds, lakes, and rivers. Transpiration and evaporation are usually considered together as ET at the watershed scale. ET dominates the water balance and controls the availability of water for soil moisture storage, groundwater recharge, and runoff. P E T denotes the rate of water loss to the atmosphere when not limited by water supply. In contrast, actual evapotranspiration (AET) is the actual rate of water loss to the atmosphere, constrained by the amount of water available from precipitation and irrigation [5].
Precipitation and temperature are the historical, observed, and future projected weather parameters for this study. P E T is estimated using temperature, as it is the available weather parameter for the P E T calculation, along with expected solar radiation, which is based on the study area’s latitude and season.
P E T can be estimated from the reference crop evapotranspiration, E T o , using a crop coefficient, K c , as shown in Equation (A1). In this study, K c = 1.0 and P E T = E T o , so the calculated future P E T is primarily dependent on the projected future temperature.
A modified version of the Hargreaves–Samani 1985 (HS85) equation [52,53] from Ref. [54] is used to estimate E T o , with Equation (A2), from the daily average temperature, T a v e , calculated using Equation (A3). Equation (A2) is the modified version of the HS85 equation, and the modification involves the use of the monthly-average difference in the daily maximum and minimum temperatures rather than the annual difference.
P E T = K c E T o
E T o = 0.0023 S o δ ¯ T 0.5 T a v e + 17.8
Equation (A2) provides the reference crop evapotranspiration, E T o , in millimeters per day. In this equation, S o represents the water equivalent of extraterrestrial radiation in millimeters per day. δ ¯ T denotes the difference between the monthly-average daily maximum temperature, T ¯ m a x , and the monthly-average daily minimum temperature, T ¯ m i n , as shown in Equation (A4). All temperature values in these equations are in degrees Celsius.
T a v e = 0.5 T m a x T m i n
T m a x denotes the daily maximum temperature, and T m i n denotes the daily minimum temperature.
δ ¯ T 0.5 = T ¯ m a x T ¯ m i n
The water equivalent of extraterrestrial radiation in millimeters per day, S o , is calculated using Equation (A5), where d r denotes the relative distance between the earth and the Sun, as derived from Equation (A6), ω s denotes the sunset hour angle in radians using Equation (A7), ϕ denotes the site latitude in radians, and δ denotes the solar declination in radians from Equation (A8).
S o = 15.392 d r ω s sin ϕ sin δ + cos ϕ cos δ sin ω s
d r = 1 + 0.033 cos 2 π 365 J
J denotes the Julian day number.
ω s = arccos tan ϕ tan δ
δ = 0.4093 sin 2 π 365 J 1.405

Appendix A.3. Conditional Temperature Formulation

In the weather generators used in this study, air temperature is calculated as conditional upon the precipitation state. This conditional formulation is presented in Equations (A9)–(A14). The day of the year mean, μ , and standard deviation, σ , in Equation (A9) for each state were determined using Fourier series smoothing—or low-pass filtering—of the day of the year mean and standard deviation series derived from data. The smoothed mean series was subtracted from the original data series, and the smoothed standard deviation series was used to normalize the result to produce Z-scaled residual elements, z k . Residual elements are used to calculate M 0 , Equation (A13), and M 1 , Equation (A14), matrices which are used to calculate the A, Equation (A11), and B, Equation (A12), matrices [40,42].
T k t = μ k , 0 t + σ k , 0 t z k t if day is dry μ k , 1 t + σ k , 1 t z k t if day is wet
t denotes the Julian daytime index. k denotes the index for the number of non-precipitation weather variables. k , 0 denotes a dry-state non-precipitation weather variable, and 0 signifies the dry state. k , 1 denotes a wet-state non-precipitation weather variable, and 1 signifies the wet state.
z t = A z t 1 + B ϵ t
ϵ signifies a k-dimensional vector of independent standard normal variables that provides white-noise forcing for each variable.
A = M 1 M 0 1
M 0 denotes the lag 0 covariance matrix from Equation (A13), and M 1 denotes the lag 1 covariance matrix from Equation (A14).
B B T = M 0 M 1 M 0 1 M 1 T
M 0 = 1 ρ 0 1 , 2 ρ 0 2 , 1 1
ρ 0 denotes the lag 0 cross-correlation coefficient between variables.
M 1 = ρ 1 1 , 1 ρ 1 1 , 2 ρ 1 2 , 1 ρ 1 2 , 2
ρ 1 denotes the lag 1 cross-correlation coefficient between variables.

Appendix A.4. Calibration Parameters

A total of 94 parameters are adjusted during calibration: 4 parameters are additive scalar temperature factors, as per Table A1; 6 parameters define the upper bounds for extreme event magnitudes in Table A2; 24 parameters (12 months × 2 parameters) determine the dry-state spell length distributions, detailed in Table A3; another 24 parameters 12 months × 2 parameters) are for wet-state spell length distributions, as shown in Table A4. Additionally, 36 parameters (12 months × 3 parameters) are set for precipitation intensity distributions, as seen in Table A5.
Moreover, 13 observations are used for targets, as shown in Table A6.
Table A1. Additive scalar temperature parameter specifications for calibration and “best-fit” values.
Table A1. Additive scalar temperature parameter specifications for calibration and “best-fit” values.
Parameter NameDescriptionTransformChange LimitInitial ValueLower BoundUpper BoundGroupCalibrated
parnme partransparchglimparval1parlbndparubndpargpFinal Value
tmax_wet_add C 0 , 1 Equation (2)logfactor5.12.08.0temp5.1
tmax_dry_add C 0 , 0 Equation (2)logfactor6.12.08.0temp6.9
tmin_wet_add C 1 , 1 Equation (2)logfactor0.90.13.0temp0.9
tmin_dry_add C 1 , 0 Equation (2)logfactor0.90.13.0temp0.8
Table A2. Extreme event scalar temperature parameter specifications for calibration and “best-fit” values.
Table A2. Extreme event scalar temperature parameter specifications for calibration and “best-fit” values.
Parameter NameDescriptionTransformChange LimitInitial ValueLower BoundUpper BoundGroupCalibrated
parnme partransparchglimparval1parlbndparubndpargpFinal Value
ev_2yr_max2-yr, upperlogfactor148.7105.0250.0event153.7
ev_5yr_max5-yr, upperlogfactor240.4150.0250.0event247.6
ev_10yr_max10-yr, upperlogfactor252.5190.0350.0event255.7
ev_25yr_max25-yr, upperlogfactor288.6250.0400.0event290.9
ev_50yr_max50-yr, upperlogfactor419.6300.0500.0event415.5
ev_100yr_max100-yr, upperlogfactor506.1370.0550.0event498.1
Table A3. Dry-state parameter specifications for calibration and “best-fit” values.
Table A3. Dry-state parameter specifications for calibration and “best-fit” values.
Parameter NameDescriptionTransformChange LimitInitial ValueLower BoundUpper BoundGroupCalibrated
parnme partransparchglimparval1parlbndparubndpargpFinal Value
m1_drysl_nJan, Nlogfactor4.12852.506.00dry3.9152
m1_drysl_pJan, Plogfactor0.28380.130.50dry0.2978
m2_drysl_nFeb, Nlogfactor5.26573.007.00dry5.3127
m2_drysl_pFeb, Plogfactor0.19700.130.50dry0.1989
m3_drysl_nMar, Nlogfactor3.81752.506.00dry3.6036
m3_drysl_pMar, Plogfactor0.34130.150.50dry0.3428
m4_drysl_nApr, Nlogfactor3.09792.506.00dry2.7049
m4_drysl_pApr, Plogfactor0.31540.130.50dry0.3296
m5_drysl_nMay, Nlogfactor6.53472.507.00dry6.9531
m5_drysl_pMay, Plogfactor0.31660.150.50dry0.3176
m6_drysl_nJun, Nlogfactor5.47293.007.00dry5.0589
m6_drysl_pJun, Plogfactor0.30720.130.55dry0.3010
m7_drysl_nJul, Nlogfactor6.08533.008.00dry6.0960
m7_drysl_pJul, Plogfactor0.36100.130.50dry0.3670
m8_drysl_nAug, Nlogfactor3.05762.506.00dry3.1775
m8_drysl_pAug, Plogfactor0.48440.130.55dry0.5094
m9_drysl_nSep, Nlogfactor4.06053.008.00dry3.7355
m9_drysl_pSep, Plogfactor0.24660.130.50dry0.2371
m10_drysl_nOct, Nlogfactor4.52882.506.00dry4.6063
m10_drysl_pOct, Plogfactor0.21570.130.55dry0.2057
m11_drysl_nNov, Nlogfactor3.37733.007.00dry3.0000
m11_drysl_pNov, Plogfactor0.17100.130.50dry0.1761
m12_drysl_nDec, Nlogfactor4.36913.007.00dry3.7565
m12_drysl_pDec, Plogfactor0.38020.100.50dry0.4118
Table A4. Wet-state parameter specifications for calibration and “best-fit” values.
Table A4. Wet-state parameter specifications for calibration and “best-fit” values.
Parameter NameDescriptionTransformChange LimitInitial ValueLower BoundUpper BoundGroupCalibrated
parnme partransparchglimparval1parlbndparubndpargpFinal Value
m1_wetsl_nJan, Nlogfactor4.35621.005.00wet4.5109
m1_wetsl_pJan, Plogfactor0.66880.250.75wet0.6452
m2_wetsl_nFeb, Nlogfactor2.28291.005.00wet2.4751
m2_wetsl_pFeb, Plogfactor0.68750.300.80wet0.6697
m3_wetsl_nMar, Nlogfactor1.64591.006.00wet1.6756
m3_wetsl_pMar, Plogfactor0.49560.250.70wet0.4655
m4_wetsl_nApr, Nlogfactor2.29121.005.00wet2.5563
m4_wetsl_pApr, Plogfactor0.68790.300.80wet0.6366
m5_wetsl_nMay, Nlogfactor3.62490.804.00wet3.4692
m5_wetsl_pMay, Plogfactor0.59190.200.70wet0.6070
m6_wetsl_nJun, Nlogfactor2.82041.005.00wet3.1153
m6_wetsl_pJun, Plogfactor0.41910.250.70wet0.3393
m7_wetsl_nJul, Nlogfactor1.78901.005.00wet1.8310
m7_wetsl_pJul, Plogfactor0.46470.200.70wet0.4184
m8_wetsl_nAug, Nlogfactor1.78921.005.00wet1.7144
m8_wetsl_pAug, Plogfactor0.62890.250.75wet0.6526
m9_wetsl_nSep, Nlogfactor2.38950.804.00wet2.3559
m9_wetsl_pSep, Plogfactor0.37220.300.80wet0.3354
m10_wetsl_nOct, Nlogfactor2.32311.005.00wet2.3811
m10_wetsl_pOct, Plogfactor0.56220.250.70wet0.5459
m11_wetsl_nNov, Nlogfactor2.13651.006.00wet2.1385
m11_wetsl_pNov, Plogfactor0.64720.300.90wet0.6513
m12_wetsl_nDec, Nlogfactor2.38520.804.00wet2.4403
m12_wetsl_pDec, Plogfactor0.71260.300.90wet0.6922
Table A5. Intensity parameter specifications for calibration and “best-fit” values.
Table A5. Intensity parameter specifications for calibration and “best-fit” values.
Parameter NameDescriptionTransformChange LimitInitial ValueLower BoundUpper BoundGroupCalibrated
parnme partransparchglimparval1parlbndparubndpargpFinal Value
m1_pdep_aJan, alogfactor0.76800.602.00wet0.7837
m1_pdep_cJan, clogfactor1.36500.602.50wet1.3476
m1_pdep_scaJan, scalelogfactor5.24624.0010.00wet5.6106
m2_pdep_aFeb, alogfactor0.99320.701.50wet1.0628
m2_pdep_cFeb, clogfactor1.39190.753.00wet1.3411
m2_pdep_scaFeb, scalelogfactor6.10455.0012.00wet6.3915
m3_pdep_aMar, alogfactor1.08210.752.00wet1.1007
m3_pdep_cMar, clogfactor1.34070.753.00wet1.2724
m3_pdep_scaMar, scalelogfactor8.09104.0010.00wet8.3487
m4_pdep_aApr, alogfactor1.04760.752.00wet1.1018
m4_pdep_cApr, clogfactor1.23210.753.00wet1.2110
m4_pdep_scaApr, scalelogfactor6.77184.0010.00wet6.9914
m5_pdep_aMay, alogfactor1.14720.601.50wet1.1768
m5_pdep_cMay, clogfactor1.60420.753.00wet1.5349
m5_pdep_scaMay, scalelogfactor7.29015.0012.00wet7.5088
m6_pdep_aJun, alogfactor1.44060.601.60wet1.4941
m6_pdep_cJun, clogfactor1.40840.602.50wet1.3724
m6_pdep_scaJun, scalelogfactor10.02584.0012.00wet10.5265
m7_pdep_aJul, alogfactor1.00640.601.50wet1.0484
m7_pdep_cJul, clogfactor1.50920.602.50wet1.4917
m7_pdep_scaJul, scalelogfactor9.50835.0012.00wet9.7313
m8_pdep_aAug, alogfactor0.86420.751.60wet0.8287
m8_pdep_cAug, clogfactor1.62460.602.50wet1.6187
m8_pdep_scaAug, scalelogfactor8.68945.0012.00wet8.6297
m9_pdep_aSep, alogfactor1.07260.751.60wet1.1017
m9_pdep_cSep, clogfactor1.45730.602.50wet1.4268
m9_pdep_scaSep, scalelogfactor9.49305.0012.00wet10.0139
m10_pdep_aOct, alogfactor1.55570.751.60wet1.5368
m10_pdep_cOct, clogfactor1.29890.502.50wet1.2947
m10_pdep_scOct, scalelogfactor9.64084.0010.00wet10.0000
m11_pdep_aNov, alogfactor0.77660.701.60wet0.7815
m11_pdep_cNov, clogfactor1.39030.703.00wet1.3964
m11_pdep_scNov, scalelogfactor6.77975.0012.00wet6.7561
m12_pdep_aDec, alogfactor0.76860.701.60wet0.7952
m12_pdep_cDec, clogfactor1.35110.753.00wet1.3694
m12_pdep_scDec, scalelogfactor5.36364.0010.00wet5.5408
Table A6. Target specifications and calibrated model simulated values.
Table A6. Target specifications and calibrated model simulated values.
Observation NameDescriptionObserved ValueWeightGroupSimulated
obsnme obsvalweightobsgnme
ann_ave_pre_depAnnual average P782100.0annpre780
mon_1_cum_probJan F0.14910,000.0spei0.157
mon_2_cum_probFeb F0.14910,000.0spei0.162
mon_3_cum_probMar F0.14910,000.0spei0.129
mon_4_cum_probApr F0.14910,000.0spei0.172
mon_5_cum_probMay F0.14910,000.0spei0.162
mon_6_cum_probJun F0.14910,000.0spei0.104
mon_7_cum_probJul F0.14910,000.0spei0.170
mon_8_cum_probAug F0.14910,000.0spei0.128
mon_9_cum_probSep F0.14910,000.0spei0.133
mon_10_cum_probOct F0.14910,000.0spei0.180
mon_11_cum_probNov F0.14910,000.0spei0.145
mon_12_cum_probDec F0.14910,000.0spei0.142

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Figure 1. The study area is the Frio River watershed or basin near Uvalde, Texas (TX), USA. Uvalde is 134 km (83 mi) west of San Antonio, TX. Two different gridded weather data products are used in this study: (1) Daymet v4, as discussed in Section 2.2, and (2) LOCA2, as discussed in Section 2.3. The study area is important for water budgeting because the Frio and Dry Frio Rivers cross the Balcones Fault Zone (BFZ) Edwards Aquifer Recharge Zone in the southern portion of the basin and provide direct communication between surface and subsurface water.
Figure 1. The study area is the Frio River watershed or basin near Uvalde, Texas (TX), USA. Uvalde is 134 km (83 mi) west of San Antonio, TX. Two different gridded weather data products are used in this study: (1) Daymet v4, as discussed in Section 2.2, and (2) LOCA2, as discussed in Section 2.3. The study area is important for water budgeting because the Frio and Dry Frio Rivers cross the Balcones Fault Zone (BFZ) Edwards Aquifer Recharge Zone in the southern portion of the basin and provide direct communication between surface and subsurface water.
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Figure 2. Frio basin observed weather parameter (Climate Normals) from 1991 to 2020 compared to LOCA2 Climate Normals from 2031–2060. “Precip.” denotes the total precipitation depth for the month. “Max. Temp.” denotes the daily maximum temperature, and “Min. Temp.” denotes the daily minimum temperature. Climate Normals are the monthly averages of the weather parameters across the specified 30-year period. Temperature is expected to consistently increase for the 2031–2060 period compared to the 1991–2020 period. Precipitation depth is expected to decrease slightly for the 2031–2060 period relative to the 1991–2020 period.
Figure 2. Frio basin observed weather parameter (Climate Normals) from 1991 to 2020 compared to LOCA2 Climate Normals from 2031–2060. “Precip.” denotes the total precipitation depth for the month. “Max. Temp.” denotes the daily maximum temperature, and “Min. Temp.” denotes the daily minimum temperature. Climate Normals are the monthly averages of the weather parameters across the specified 30-year period. Temperature is expected to consistently increase for the 2031–2060 period compared to the 1991–2020 period. Precipitation depth is expected to decrease slightly for the 2031–2060 period relative to the 1991–2020 period.
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Figure 3. The LOCA2 annual average temperature cone of uncertainty along with the observed annual average temperature for the Frio basin. The annual average temperature is calculated as the average across the year of the daily average temperature, as detailed in Appendix A.2. Temperature is projected to consistently increase in the future. By 2065, the expected annual average temperature values are projected to be about 3 °C higher than the observed annual average temperatures in the early 2020s. “LOCA2 5th to 95th envelope” represents the range of temperature magnitudes for a given year, bounded by the 5th and 95th percentile values, across the 23 ensemble members. The percentile envelopes would be smoother with more realizations or ensemble members.
Figure 3. The LOCA2 annual average temperature cone of uncertainty along with the observed annual average temperature for the Frio basin. The annual average temperature is calculated as the average across the year of the daily average temperature, as detailed in Appendix A.2. Temperature is projected to consistently increase in the future. By 2065, the expected annual average temperature values are projected to be about 3 °C higher than the observed annual average temperatures in the early 2020s. “LOCA2 5th to 95th envelope” represents the range of temperature magnitudes for a given year, bounded by the 5th and 95th percentile values, across the 23 ensemble members. The percentile envelopes would be smoother with more realizations or ensemble members.
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Figure 4. The LOCA2 annual total precipitation depth cone of uncertainty along with the observed annual precipitation depth for the Frio basin. The annual precipitation depth is projected to remain similar to the historically observed annual precipitation depth with an expectation of a slight decrease in magnitude. “LOCA2 25th to 75th envelope” represents the precipitation depths for a given year bounded by the 25th percentile and 75th percentile values. There are 23 ensemble members. The percentile envelopes would be smoother if more realizations or ensemble members were employed.
Figure 4. The LOCA2 annual total precipitation depth cone of uncertainty along with the observed annual precipitation depth for the Frio basin. The annual precipitation depth is projected to remain similar to the historically observed annual precipitation depth with an expectation of a slight decrease in magnitude. “LOCA2 25th to 75th envelope” represents the precipitation depths for a given year bounded by the 25th percentile and 75th percentile values. There are 23 ensemble members. The percentile envelopes would be smoother if more realizations or ensemble members were employed.
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Figure 5. Standardizing transform that is the basis of the SPEI and SPI calculations. The example transform provided in this figure is for the SPEI. The left-side plot displays the probability distribution fit to a collection of cumulative monthly totals for the deficit for SPEI (precipitation is used for SPI). A log-logistic distribution is used for the SPEI calculation, and a gamma distribution is used for the SPI calculation. Cumulative probability, F, calculated from the fitted distribution is used to transform to a Z-score, Z, which identifies the number of standard deviations from the mean in the standard normal distribution. The Z value on the right-hand panel is the calculated SPEI value; reproduced from Ref. [35].
Figure 5. Standardizing transform that is the basis of the SPEI and SPI calculations. The example transform provided in this figure is for the SPEI. The left-side plot displays the probability distribution fit to a collection of cumulative monthly totals for the deficit for SPEI (precipitation is used for SPI). A log-logistic distribution is used for the SPEI calculation, and a gamma distribution is used for the SPI calculation. Cumulative probability, F, calculated from the fitted distribution is used to transform to a Z-score, Z, which identifies the number of standard deviations from the mean in the standard normal distribution. The Z value on the right-hand panel is the calculated SPEI value; reproduced from Ref. [35].
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Figure 6. Schematic of weather generator (WG) implementation, including extreme events. WGs facilitate the stochastic simulation of precipitation occurrence and intensity, as well as maximum and minimum daily temperature. The precipitation occurrence process is represented using an alternating state, spell length approach based on negative binomial distributions. Precipitation intensity is represented by daily, wet-state precipitation depth sampled from two-parameter gamma distributions. Simulated air temperature is conditioned on the current state and calculated using a first-order vector autoregression. Extreme events are incorporated into this formulation, with events implemented using a Poisson distribution for interarrival times of event occurrence and a uniform distribution for event magnitude.
Figure 6. Schematic of weather generator (WG) implementation, including extreme events. WGs facilitate the stochastic simulation of precipitation occurrence and intensity, as well as maximum and minimum daily temperature. The precipitation occurrence process is represented using an alternating state, spell length approach based on negative binomial distributions. Precipitation intensity is represented by daily, wet-state precipitation depth sampled from two-parameter gamma distributions. Simulated air temperature is conditioned on the current state and calculated using a first-order vector autoregression. Extreme events are incorporated into this formulation, with events implemented using a Poisson distribution for interarrival times of event occurrence and a uniform distribution for event magnitude.
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Figure 7. Frio basin calibrated weather generator (WG) Climate Normals from 2031–2060 compared to observed 1991–2020 Climate Normals and LOCA2 projected Climate Normals for 2031–2060. “Precip.” is the total precipitation depth, P, for the month. “Max. Temp.” is the daily maximum temperature, and “Min. Temp.” is the daily minimum temperature. Climate Normals are the monthly averages of these weather parameters across the specified 30-year period. Temperature is expected to consistently increase for 2031–2060 compared to 1991–2020.
Figure 7. Frio basin calibrated weather generator (WG) Climate Normals from 2031–2060 compared to observed 1991–2020 Climate Normals and LOCA2 projected Climate Normals for 2031–2060. “Precip.” is the total precipitation depth, P, for the month. “Max. Temp.” is the daily maximum temperature, and “Min. Temp.” is the daily minimum temperature. Climate Normals are the monthly averages of these weather parameters across the specified 30-year period. Temperature is expected to consistently increase for 2031–2060 compared to 1991–2020.
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Figure 8. WG annual average temperature cone of uncertainty. The annual average temperature is the average across the year of the daily average temperature calculated per Appendix A.2. The WG formulation is stationary in time; consequently, the cone of uncertainty is flat. The mean temperature in this plot is approximately equal to the mean temperature during the 2050s in the LOCA2 cone of uncertainty in Figure 3. The “5th to 95th envelope” refers to the temperature magnitudes for a given year bounded by the 5th percentile and 95th percentile values. Similarly, the “25th to 75th envelope” refers to the temperature magnitudes for a given year bounded by the 25th percentile and 75th percentile values. A total of 1000 stochastic realizations are used, creating relatively smooth value distributions.
Figure 8. WG annual average temperature cone of uncertainty. The annual average temperature is the average across the year of the daily average temperature calculated per Appendix A.2. The WG formulation is stationary in time; consequently, the cone of uncertainty is flat. The mean temperature in this plot is approximately equal to the mean temperature during the 2050s in the LOCA2 cone of uncertainty in Figure 3. The “5th to 95th envelope” refers to the temperature magnitudes for a given year bounded by the 5th percentile and 95th percentile values. Similarly, the “25th to 75th envelope” refers to the temperature magnitudes for a given year bounded by the 25th percentile and 75th percentile values. A total of 1000 stochastic realizations are used, creating relatively smooth value distributions.
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Figure 9. WG annual precipitation depth cone of uncertainty. The mean annual precipitation depth in this plot is lower than the 10-year rolling average, observed precipitation depth in Figure 4. The “5th to 95th envelope” denotes the precipitation magnitudes for a given year bounded by the 5th percentile and 95th percentile values. Similarly, the “25th to 75th envelope” denotes the precipitation magnitudes for a given year bounded by the 25th percentile and 75th percentile values. A total of 1000 stochastic realizations are used, creating relatively smooth value distributions.
Figure 9. WG annual precipitation depth cone of uncertainty. The mean annual precipitation depth in this plot is lower than the 10-year rolling average, observed precipitation depth in Figure 4. The “5th to 95th envelope” denotes the precipitation magnitudes for a given year bounded by the 5th percentile and 95th percentile values. Similarly, the “25th to 75th envelope” denotes the precipitation magnitudes for a given year bounded by the 25th percentile and 75th percentile values. A total of 1000 stochastic realizations are used, creating relatively smooth value distributions.
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Figure 10. Comparison of the distribution of annual precipitation depth, P, among 2031–2060 WG projections, 2031–2060 LOCA2 projections, and 1991–2020 observations. The mean annual P is identified with green triangles and is the smallest in the LOCA2 2031–2060 projections. It is approximately equal between WG 2031–2060 projections and observed 1991–2020 values. Outliers—or extreme P years—are identified with the black diamonds. The WG 2031–2060 distribution has the most outliers because of the use of extreme events in the WG formulation.
Figure 10. Comparison of the distribution of annual precipitation depth, P, among 2031–2060 WG projections, 2031–2060 LOCA2 projections, and 1991–2020 observations. The mean annual P is identified with green triangles and is the smallest in the LOCA2 2031–2060 projections. It is approximately equal between WG 2031–2060 projections and observed 1991–2020 values. Outliers—or extreme P years—are identified with the black diamonds. The WG 2031–2060 distribution has the most outliers because of the use of extreme events in the WG formulation.
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Figure 11. Comparison of the SPEI drought index values for the observed 1993–2022, 3-month cumulative D values: Panel (a) SPEI based on 1981–2010 observations, Panel (b) SPEI based on LOCA2 projected 2031–2060 conditions, and Panel (c) SPEI based on WG-projected 2031–2060 conditions. An SPEI 1.5 represents severe drought conditions. According to the observed 1981–2010 climate description in Panel (a), severe drought conditions occurred 17 times from 1993 to 2022 with a minimum calculated SPEI of 2.1 . Using LOCA2 2031–2060 conditions, severe drought occurred four times between 1993 and 2022, with a minimum SPEI of 1.9 . For the 1993–2022 observations analyzed using WG 2031–2060 conditions, no severe droughts occurred, and the minimum SPEI was 1.4 . This comparison demonstrates that the WG 2031–2060 climate description is significantly warmer and drier on average than the LOCA2 2031–2060 description.
Figure 11. Comparison of the SPEI drought index values for the observed 1993–2022, 3-month cumulative D values: Panel (a) SPEI based on 1981–2010 observations, Panel (b) SPEI based on LOCA2 projected 2031–2060 conditions, and Panel (c) SPEI based on WG-projected 2031–2060 conditions. An SPEI 1.5 represents severe drought conditions. According to the observed 1981–2010 climate description in Panel (a), severe drought conditions occurred 17 times from 1993 to 2022 with a minimum calculated SPEI of 2.1 . Using LOCA2 2031–2060 conditions, severe drought occurred four times between 1993 and 2022, with a minimum SPEI of 1.9 . For the 1993–2022 observations analyzed using WG 2031–2060 conditions, no severe droughts occurred, and the minimum SPEI was 1.4 . This comparison demonstrates that the WG 2031–2060 climate description is significantly warmer and drier on average than the LOCA2 2031–2060 description.
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Figure 12. Comparison of SPI drought index values for the observed 1993–2022 3-month cumulative P among: Panel (a) SPI based on 1981–2010 observations, Panel (b) SPI based on LOCA2 projected 2031–2060 conditions, and Panel (c) SPI based on WG-projected 2031–2060 conditions. “Severe” wet periods are identified with SPI ≥ 1.5. According to the observed 1981–2010 climate description in Panel (a), severe wet conditions occurred 17 times from 1993 to 2022 with a maximum calculated SPI of 3.1 . Using LOCA2 2031–2060 conditions, severe wet periods occurred 37 times between 1993 and 2022 with a maximum SPI of 3.2 . Looking at the 1993–2022 observations using WG 2031–2060 conditions, severe wet periods occurred 41 times and the maximum SPI was 5.3 . These results agree with the comparisons among the three datasets for precipitation provided in Figure 7 and Figure 10.
Figure 12. Comparison of SPI drought index values for the observed 1993–2022 3-month cumulative P among: Panel (a) SPI based on 1981–2010 observations, Panel (b) SPI based on LOCA2 projected 2031–2060 conditions, and Panel (c) SPI based on WG-projected 2031–2060 conditions. “Severe” wet periods are identified with SPI ≥ 1.5. According to the observed 1981–2010 climate description in Panel (a), severe wet conditions occurred 17 times from 1993 to 2022 with a maximum calculated SPI of 3.1 . Using LOCA2 2031–2060 conditions, severe wet periods occurred 37 times between 1993 and 2022 with a maximum SPI of 3.2 . Looking at the 1993–2022 observations using WG 2031–2060 conditions, severe wet periods occurred 41 times and the maximum SPI was 5.3 . These results agree with the comparisons among the three datasets for precipitation provided in Figure 7 and Figure 10.
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Table 1. Drought intensity definitions for SPI values from Ref. [34].
Table 1. Drought intensity definitions for SPI values from Ref. [34].
SPI ValuesDrought CategoryTime in Category 1
0 to −0.99Mild drought≈24%
−1.00 to −1.49Moderate drought9.2%
−1.50 to −1.99Severe drought4.4%
≤−2Extreme drought2.3%
1 SPI values conceptually correspond to standard deviations from the mean for the standard normal distribution, and “Time in Category” corresponds to one-sided confidence intervals.
Table 2. Extreme event configuration and estimated 24-h point depths for the Frio basin.
Table 2. Extreme event configuration and estimated 24-h point depths for the Frio basin.
Recurrence IntervalUniform Distribution for Event Magnitude24-h Event 1
Event Label(Year)Lower Bound (mm)Upper Bound (mm) 2Depth (mm)
2-year296105 to 25096
5-year5141135 to 250141
10-year10179190 to 350179
25-year25236250 to 400236
50-year50285300 to 500285
100-year100343370 to 550343
1 The 24-h event magnitude for the basin centroid location from Ref. [44]. 2 The upper bound varies across the stated range as part of the weather generator calibration.
Table 3. Summer 2022 drought index-related values for the Frio basin.
Table 3. Summer 2022 drought index-related values for the Frio basin.
May 2022Jun 2022Jul 2022Aug 2022Sep 2022
3-month D, mm−400−473−540−434−367
corresponding F0.090.060.0300.250.43
historical SPEI−1.4−1.6−1.9−0.7−0.2
3-month P, mm879388175183
corresponding F0.110.080.0520.460.59
historical SPI−1.2−1.4−1.6−0.10.2
Table 4. Frio basin drought-related WG calibration targets from weather attribution with results.
Table 4. Frio basin drought-related WG calibration targets from weather attribution with results.
Month3-Month D for Historical F = 0.030 Target FCalibrated WG Results
mm 5 × 0.030 Simulated F # of Times
Jan−2190.1490.1575.3
Feb−2210.1490.1625.4
Mar−2830.1490.1294.3
Apr−3600.1490.1725.8
May−4640.1490.1625.4
Jun−5090.1490.1043.5
Jul−5400.1490.1705.7
Aug−5540.1490.1284.3
Sep−5280.1490.1334.5
Oct−4180.1490.1806.0
Nov−3280.1490.1454.9
Dec−2700.1490.1424.8
Table 5. Frio basin annual average climate parameters.
Table 5. Frio basin annual average climate parameters.
Climate ParameterDatasetAnnual Average Depth mm
Observed 1991–2020782
Precipitation PWG 2031–2060780
LOCA2 2031–2060688
Observed 1991–20201532
E T o = P E T WG 2031–20601996
LOCA2 2031–20601659
Observed 1991–2020−750
Deficit DWG 2031–2060−1216
LOCA2 2031–2060−970
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