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**Hydrology and Earth System Sciences**
An interactive open-access journal of the European Geosciences Union

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**Research article**
20 Apr 2018

**Research article** | 20 Apr 2018

Analytical flow duration curves for summer streamflow in Switzerland

^{1}School of Architecture, Civil and Environmental Engineering (ENAC), École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland^{2}Instituto Superior Técnico, Technical University of Lisbon, Lisbon, Portugal^{3}Faculty of Geosciences and Environment, University of Lausanne, Lausanne, Switzerland^{4}Dipartimento di Ingegneria Civile Edile e Ambientale, Universitá degli studi di Padova, Padua, Italy

^{1}School of Architecture, Civil and Environmental Engineering (ENAC), École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland^{2}Instituto Superior Técnico, Technical University of Lisbon, Lisbon, Portugal^{3}Faculty of Geosciences and Environment, University of Lausanne, Lausanne, Switzerland^{4}Dipartimento di Ingegneria Civile Edile e Ambientale, Universitá degli studi di Padova, Padua, Italy

**Correspondence**: Ana Clara Santos (anaclara.santos@epfl.ch)

**Correspondence**: Ana Clara Santos (anaclara.santos@epfl.ch)

Abstract

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This paper proposes a systematic assessment of the performance of an analytical modeling framework for streamflow probability distributions for a set of 25 Swiss catchments. These catchments show a wide range of hydroclimatic regimes, including namely snow-influenced streamflows. The model parameters are calculated from a spatially averaged gridded daily precipitation data set and from observed daily discharge time series, both in a forward estimation mode (direct parameter calculation from observed data) and in an inverse estimation mode (maximum likelihood estimation). The performance of the linear and the nonlinear model versions is assessed in terms of reproducing observed flow duration curves and their natural variability. Overall, the nonlinear model version outperforms the linear model for all regimes, but the linear model shows a notable performance increase with catchment elevation. More importantly, the obtained results demonstrate that the analytical model performs well for summer discharge for all analyzed streamflow regimes, ranging from rainfall-driven regimes with summer low flow to snow and glacier regimes with summer high flow. These results suggest that the model's encoding of discharge-generating events based on stochastic soil moisture dynamics is more flexible than previously thought. As shown in this paper, the presence of snowmelt or ice melt is accommodated by a relative increase in the discharge-generating frequency, a key parameter of the model. Explicit quantification of this frequency increase as a function of mean catchment meteorological conditions is left for future research.

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How to cite.

Santos, A. C., Portela, M. M., Rinaldo, A., and Schaefli, B.: Analytical flow duration curves for summer streamflow in Switzerland, Hydrol. Earth Syst. Sci., 22, 2377–2389, https://doi.org/10.5194/hess-22-2377-2018, 2018.

1 Introduction

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Knowledge of the availability and variability of daily discharges in a given stream section proves useful for many engineering applications (e.g., the design of hydropower plants or water supply systems) and for studies about stream ecology alterations and sediment transport or about water quality and allocation (Basso et al., 2015; Ceola et al., 2010; Searcy, 1959; Vogel and Fennessey, 1995). For many such applications, knowledge of the probability distribution of daily discharges rather than of their exact temporal occurrence is sufficient.

In hydrology, the probability distribution of daily discharges is traditionally not represented as a probability density function (pdf), but in terms of flow duration curves (FDCs) that assign an exceedance probability to each discharge value (Vogel and Fennessey, 1994) and that correspond to the complement of the cumulative distribution function (cdf).

Different methods exist to estimate FDCs (ie. to estimate their shape), the most straightforward method being the assignment of empirical probabilities to observed ranked data (yielding empirical FDCs; Vogel and Fennessey, 1994). FDCs can also be obtained from statistical methods that relate the FDC shape to catchment characteristics (Castellarin et al., 2013).

An important category of FDC models are process-based models that combine climate controls and catchment characteristics to estimate the shape of FDCs. Such models describe the shape of FDCs either based on long-term simulations of the system behavior or based on a direct parameterization of the FDC shape as a function of key hydrological controls. One such model is the model developed by Botter et al. (2007c), who derived an analytical description of streamflow distributions as the result of subsurface flow pulses triggered by stochastic rainfall and censored by the soil moisture dynamics. The resulting streamflow distribution is characterized by only a few parameters: the mean rainfall depth and the frequency of rainfall events that produce discharge, the area of the catchment and the mean residence time of the catchment.

This modeling framework has been applied successfully for a range of case studies in Italy (Botter et al., 2007c, 2009; Ceola et al., 2010; Schaefli et al., 2013), Switzerland (Basso et al., 2015; Doulatyari et al., 2017; Schaefli et al., 2013) and the US (Botter et al., 2007a, 2013; Ceola et al., 2010). Müller et al. (2014) expanded the framework to seasonally dry climates with an application in Nepal. According to Müller and Thompson (2016), the benefits of such a process-based approach, as opposed to purely statistical or empirical methods, can be summarized as follows: (i) it provides an explicit link between the FDC shape, rainfall characteristics and catchment recession characteristics rather than an empirical or statistical link to regional FDC shapes; (ii) the method is applicable to periods characterized by different meteorological conditions, thanks to the explicit treatment of rainfall and evapotranspiration characteristics.

The original model framework was developed for rainfall-driven catchments that show a linear recession behavior. Besides the aforementioned extension to seasonally dry climates, the framework has namely been extended to nonlinear recessions (Botter et al., 2009) and to the description of winter low flow resulting from seasonal snow accumulation (Schaefli et al., 2013).

In the previous applications of the model, the focus was generally on the study of signatures of discharge regimes under different climates and landscape conditions (Botter et al., 2007a, 2013), where the shape of the pdf was more important than the accuracy of the predicted discharge probabilities. Furthermore, all previous applications deliberately excluded all catchments or seasons that were snowmelt affected (Botter et al., 2007a, 2013; Ceola et al., 2010; Doulatyari et al., 2015).

The objective of this research is to assess and compare the performance of the model in its linear and nonlinear forms for summer streamflows for a range of Alpine discharge regimes. The selected set of case studies covers all Swiss catchments that have a natural (unperturbed) discharge regime and long-term discharge monitoring. Compared to existing studies (e.g., Basso et al., 2015; Ceola et al., 2010; Doulatyari et al., 2017), this paper provides a systematic analysis of all model parameters and of their seasonality, and a comprehensive analysis of a wide range of discharge regimes, including namely rainfall-driven and snowfall-influenced regimes. This allows for the first detailed view of the suitability of the modeling framework for Alpine summer discharges (influenced by rain and snow) and an assessment of the model performance as a function of the discharge regime.

The paper is organized as follows: Sect. 2 provides a description of the analytical model, together with the methods adopted in this paper to estimate the model parameters and to assess the model performance, followed by a presentation of the Swiss case studies (Sect. 3). The obtained results for the linear and nonlinear model versions (Sect. 4) are discussed in Sect. 5 with a particular focus on the model performance under different hydrological regimes. The conclusions are summarized in Sect. 6.

2 Methods

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Here, we first give a short overview of the used analytic modeling framework, followed by the two different methods adopted for parameter
estimation and for model performance assessment. All methods are applied only
to the summer season (1 June to 31 August; see also Sect. 3). The model evaluation framework adopted here is synthesized in
Fig. 1, starting from the empirical cdfs as references for
performance evaluation. Next, the precipitation frequency
*λ*_{p} (Sect. 2.1) is estimated from precipitation and the discharge-producing
frequency *λ* from observed discharge (Eq. 7, Sect. 2.2). The recession parameters are obtained in forward
mode (Sect. 2.2) or inverse mode (Sect. 2.3). Based on these parameters,
the model cdf is calculated from the linear model (Eq. 4)
or from the nonlinear model (Eq. 6). The model performance
is evaluated based on two classical performance indicators and by comparison
to the natural variability of the observed cdfs (Sect. 2.4).

The analytical modeling framework of Botter et al. (2007c) for
probabilistic characterization of rainfall-driven daily discharges is based
on a soil moisture model originally proposed by
Rodriguez-Iturbe et al. (1999). This point-scale model represents the
dynamics of soil moisture as the result of a deterministic, state-dependent
loss function, combined with stochastic increments triggered by rainfall
events. Rodriguez-Iturbe et al. (1999) showed that the corresponding
spatially averaged soil moisture *s*(*t*) can be obtained from the water
balance equation as follows:

$$\begin{array}{}\text{(1)}& {\displaystyle \frac{\text{d}s\left(t\right)}{\text{d}t}}=-\mathit{\rho}\left[s\right(t\left)\right]+{\mathit{\xi}}_{\text{t}},\end{array}$$

where −*ρ*[*s*(*t*)] is the loss function, due to evapotranspiration, surface
runoff and deep percolation, and where *ξ*_{t} represents the stochastic
instantaneous increments due to infiltration from rainfall.

Botter et al. (2007c) proposed describing the dynamics of daily streamflow with a similar stochastic differential equation, supposing that rainfall acts as a stochastic forcing for discharge production and that, at the catchment scale, the water is released following a linear decay:

$$\begin{array}{}\text{(2)}& {\displaystyle \frac{\text{d}Q\left(t\right)}{\text{d}t}}=-kQ\left(t\right)+{\mathit{\xi}}_{\text{t}}^{\prime \prime},\end{array}$$

where *Q* is the daily streamflow, *k* is the inverse of the time constant
associated with the loss function and ${\mathit{\xi}}_{\text{t}}^{\prime \prime}$ is the stochastic process
associated with discharge-producing precipitation events (i.e., the sequence of
events that trigger a flow response in the river).

It is assumed here that discharge *Q* is the result of a series of rainfall
inputs (${\mathit{\xi}}_{\text{t}}^{\prime \prime}$) that deliver enough water to fill the water deficit in the
soil, i.e., that deliver enough water to raise the soil moisture level above
its retention capacity. The excess water is removed from the soil as
subsurface runoff and becomes river discharge. This description of the
streamflow response neglects any direct surface flow.

The overall rainfall forcing *ξ* is modeled as a marked Poisson process
with frequency *λ*_{p} and exponentially distributed rainfall
depths with average *α* (average rainfall on rain days). Nevertheless,
not all the rainfall events trigger streamflow responses, and the
discharge-producing precipitation events *ξ*” are also modeled as a marked
Poisson process with a decreased frequency *λ*<*λ*_{p} and the
same *α*. *λ* is influenced by the soil storage capacity and soil
drying time and can be written as (Botter et al., 2007a)

$$\begin{array}{}\text{(3)}& \mathit{\lambda}=\mathit{\eta}{\displaystyle \frac{\mathrm{exp}(-\mathit{\gamma}){\mathit{\gamma}}^{\frac{{\mathit{\lambda}}_{\text{p}}}{\mathit{\eta}}}}{\mathrm{\Gamma}({\mathit{\lambda}}_{\text{p}}/\mathit{\eta},\mathit{\gamma})}},\end{array}$$

where Γ(*a*,*b*) is a lower incomplete Gamma function with parameters *a*
and *b*, $\mathit{\eta}=E/\left(n{Z}_{\text{r}}\right({s}_{\mathrm{1}}-{s}_{\text{w}}\left)\right)$, $\mathit{\gamma}={\mathit{\gamma}}_{\text{p}}n{Z}_{\text{r}}({s}_{\mathrm{1}}-{s}_{\text{w}})$ and
${\mathit{\gamma}}_{\text{p}}=\mathrm{1}/\mathit{\alpha}$. *E* is the maximum evapotranspiration rate and
*n**Z*_{r}(*s*_{1}−*s*_{w}) synthesizes the soil volume liable to be filled by water
before drainage starts; *n* is the porosity of the soil, *Z*_{r} is the
effective soil depth, *s*_{1} is the retention capacity and *s*_{w} the permanent
wilting point.

As discussed in detail by Botter et al. (2007c), this framework results in the following probability distribution of daily discharges at the catchment scale:

$$\begin{array}{}\text{(4)}& p(Q,t\to \mathrm{\infty})={\displaystyle \frac{\mathrm{1}}{\mathrm{\Gamma}\left(\frac{\mathit{\lambda}}{k}\right)}}{\displaystyle \frac{\mathrm{1}}{Q}}{\left({\displaystyle \frac{Q}{\mathit{\alpha}kA}}\right)}^{{\scriptscriptstyle \frac{\mathit{\lambda}}{k}}}\phantom{\rule{0.33em}{0ex}}\mathrm{exp}\left(-{\displaystyle \frac{Q}{\mathit{\alpha}kA}}\right),\end{array}$$

where *A* is the catchment area. This corresponds to a Gamma distribution
with shape parameter *λ*∕*k* and a scale parameter *α**k**A*. The
corresponding expected mean discharge equals $\stackrel{\mathrm{\u203e}}{Q}=\mathit{\lambda}\mathit{\alpha}$.
The model is suitable for steady-state conditions, at the annual or seasonal
scale, depending on the temporal variability of the model parameters
(Botter et al., 2007a).

Nonlinear storage–discharge relationships at the catchment scale are commonly observed (Botter et al., 2009; Brutsaert and Nieber, 1977; Mutzner et al., 2013). Accordingly, Botter et al. (2009) proposed an extension of the above modeling framework assuming that

$$\begin{array}{}\text{(5)}& {\displaystyle \frac{\text{d}Q\left(t\right)}{\text{d}t}}=-{k}_{\text{n}}Q(t{)}^{a}+{\mathit{\xi}}_{\text{t}}^{\prime \prime},\end{array}$$

where *k*_{n} and *a* are the constants of the nonlinear recession. As for
the linear model, it is possible to obtain an equation for the pdf of the
daily discharges:

$$\begin{array}{}\text{(6)}& p(Q,t\to \mathrm{\infty})=C\left\{{\displaystyle \frac{\mathrm{1}}{{Q}^{a}}}\mathrm{exp}\left[-{\displaystyle \frac{{Q}^{\mathrm{2}-a}}{\mathit{\alpha}{k}_{\text{n}}(\mathrm{2}-a)}}+{\displaystyle \frac{{Q}^{\mathrm{1}-a}\mathit{\lambda}}{{k}_{\text{n}}(\mathrm{1}-a)}}\right]\right\},\end{array}$$

where *C* is a normalizing constant (Botter et al., 2009).

We use the term “forward parameter estimation” to emphasize that the
parameters are estimated directly from observed data, without calibration.
This method is generally used in the context of this modeling framework for
the estimation of the parameters related to the stochastic inputs
(*λ*_{p}, *α*, *λ*), and this method is always used for these
parameters in the present paper. However, the recession parameters (*k*,
*k*_{n} and *a*) are either estimated in a forward mode
(Botter et al., 2007c, 2009; Ceola et al., 2010; Schaefli et al., 2013)
or in an inverse mode (Ceola et al., 2010) (see Sect. 2.3).

The computation of the precipitation parameters first involves the
computation of a reference catchment-scale precipitation time series (here
obtained from gridded data; see Sect. 3). Then interception losses (*I*)
are subtracted from the observed daily precipitation depths. These losses are
in fact evaporated (or sublimated in case of snow) before participating to
soil moisture dynamics. Following Rodriguez-Iturbe et al. (1999),
previous model applications generally assumed that these losses are accounted
for when the frequency of precipitation events is corrected to the frequency
of discharge-producing events. In view of understanding how the model
parameters vary in space, it was decided here to treat interception losses
explicitly with minimal assumptions about this process: different maximum
interception depths are attributed to four different land covers: 4 mm for
forests, 2 mm for low vegetation, 1 mm for impervious areas and 0 mm for water
bodies (Gerrits, 2010). The catchment-scale maximum interception
depth is obtained as the land-use-weighted average of these values, but a
minimum interception depth of 1 mm is imposed. This catchment-scale
interception depth is subtracted from daily precipitation depths, assuming
that at a daily time step, all intercepted water re-evaporates during the
same time step.

Instead of correcting the frequency of precipitation events *λ*_{p}
according to Eq. (3), the frequency of
discharge-producing events *λ* is estimated directly from the
theoretical relationship between the mean discharge and the precipitation
parameters, $\stackrel{\mathrm{\u203e}}{Q}=\mathit{\lambda}\mathit{\alpha}$ (see Eq. 4).
Replacing the mean modeled discharge $\stackrel{\mathrm{\u203e}}{Q}$ with the mean observed
discharge $\stackrel{\mathrm{\u203e}}{\stackrel{\mathrm{\u0303}}{Q}}$, it follows that

$$\begin{array}{}\text{(7)}& \mathit{\lambda}={\displaystyle \frac{\mathit{\alpha}}{\stackrel{\mathrm{\u203e}}{\stackrel{\mathrm{\u0303}}{Q}}}}.\end{array}$$

Estimating *λ* from the above equation rather than directly from the
soil properties as in Eq. (3) has been shown by
Ceola et al. (2010) to provide much better results, and this method
has been used by the majority of studies since then
(e.g., Ceola et al., 2010; Botter et al., 2013; Basso et al., 2015).

The recession parameter for the linear model is calculated directly from
observed daily discharge based on a classical Brutsaert–Nieber recession
analysis
(Brutsaert and Nieber, 1977; Biswal and Marani, 2010, 2014; Mutzner et al., 2013),
considering, however, only discharges below a certain threshold, fixed to
95 %. The nonlinear recession parameters *k*_{n} and *a* are also obtained
from a recession analysis, using the same discharge threshold via
linear regression of the logarithm of ($-\text{d}Q/\text{d}t$) versus the logarithm of *Q*,
where *a* is the slope and *k*_{n} the intercept.

To objectively compare the potential of the linear and the nonlinear model
formulations to capture observed flow-duration curves, the recession
parameters for the linear model (*k*) and for the nonlinear model (*k*_{n},*a*)
are also estimated in a classical inverse estimation mode where the model
parameters are obtained by maximizing the likelihood function formulated for
the model. For the linear model, the likelihood function is obtained from the
model as follows:

$$\begin{array}{}\text{(8)}& \mathcal{L}\left(k\right|\stackrel{\mathrm{\u0303}}{Q},\mathit{\theta})=\prod _{j=\mathrm{1}}^{N}p({\stackrel{\mathrm{\u0303}}{Q}}_{j}|k,\mathit{\theta}),\end{array}$$

where the probability *p*(.) is obtained from Eq. (4) and
$\mathit{\theta}=[\mathit{\alpha},A,\mathit{\lambda}]$ is the parameter vector containing all parameters
that are estimated directly from observed data (i.e., not maximized). For the
nonlinear case, the likelihood is obtained analogously by replacing *k* with
*k*_{n} and *a* and using *p*(.) from Eq. (6).

To objectively compare different models, we propose using the Kolmogorov–Smirnov distance between the cdfs corresponding to different models (Ceola et al., 2010; Schaefli et al., 2013), i.e., the maximum difference between the values of the empirical and the modeled cumulative distributions:

$$\begin{array}{}\text{(9)}& {c}^{\text{KS}}=\underset{x}{sup}\left|F\right(\stackrel{\mathrm{\u0303}}{Q})-F(Q\left)\right|,\end{array}$$

where $F\left(\stackrel{\mathrm{\u0303}}{Q}\right)$ corresponds to the empirical cumulative distribution of
the discharges and *F*(*Q*) to the modeled cumulative distribution of the
discharges. A good model should have a low *c*^{KS} value.

This comparison of the cdfs overcomes an important limitation inherent in the comparison of analytic pdfs and empirical pdfs. In fact, the choice of the number of classes for the calculation of the empirical pdf from observed data (via a so-called frequency polygon; Naghettini, 2016) can change the shape of the empirical pdf. The problem does not arise for cdfs given their cumulative nature.

Since the nonlinear model formulation has an additional parameter, the linear and the nonlinear models are also compared based on the Akaike information criterion (Burnham and Anderson, 2004; Laio et al., 2009; Ceola et al., 2010):

$$\begin{array}{}\text{(10)}& {c}^{\text{AIC}}=\mathrm{2}n-\text{ln}\left(\widehat{\mathcal{L}}\right),\end{array}$$

where *n* is the number of parameters of the model and
ln$\left(\widehat{\mathcal{L}}\right)$ is the logarithm of the maximum likelihood function
obtained by maximizing Eq. (8). As for *c*^{KS},
a good model should have a low *c*^{AIC} value.

Based on the above criterion, we measure the relative performance increase from the linear to the nonlinear model as follows:

$$\begin{array}{}\text{(11)}& {r}^{\text{AIC}}=-\left({\displaystyle \frac{{c}_{\text{n}}^{\text{AIC}}-{c}_{\text{l}}^{\text{AIC}}}{{c}_{\text{l}}^{\text{AIC}}}}\right),\end{array}$$

where ${{c}_{\text{n}}}^{\text{AIC}}$ is the Akaike criterion for the nonlinear model
and ${c}_{\text{l}}^{\text{AIC}}$ for the linear model. Taking the opposite of the
relative difference between the Akaike criteria ensures that a higher
*r*^{AIC} value indicates a stronger performance increase (recall
that the Akaike criterion is to be minimized).

In addition, to assess the performance difference between different models, the obtained models are compared to the natural variability of the observed discharge cdfs. Therefore, an empirical long-term cdf is constructed, obtained by ranking the observed data in ascending order and dividing the rank numbers by the total sample size. Furthermore, to assess the natural yearly variability, individual cdfs are constructed for each summer season of each civil year (Vogel and Fennessey, 1994). From this collection of annual cdfs, envelopes are based on the maximum and minimum values of discharge for each probability class of the annual cdfs. A reliable model should yield a cdf contained between these curves and should be as close as possible to the long-term cdf.

3 Case studies

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In this paper, we analyze 25 Swiss catchments with areas
ranging from 1.05 to 377 km^{2} and with mean elevations ranging from
615 m a.s.l. (meters above sea level) to 2945 m a.s.l. (Table 1,
Fig. 3). These catchments
correspond to all streamflow gauging stations run by the Swiss Federal Office
for the Environment (FOEN, 2017) and that have unperturbed
discharges (i.e., minimal anthropogenic influence).

The average precipitation at the country scale is around 1300 mm yr^{−1}
(Blanc and Schädler, 2013). The complex topography leads to a high diversity of
hydrologic regimes (Weingartner and Aschwanden, 1992), which can be grouped
into (i) pluvial or rainfall-driven regimes, (ii) snow-dominated regimes and
(iii) glacier regimes. Pluvial regimes are rainfall-dominated with sporadic
snowfall events during winter; these regimes occur on the Swiss Plateau and
in the Jura region (Fig. 3). Snow-dominated regimes
result from seasonal snow cover, roughly at elevations above 900 m a.s.l. In
these catchments, solid precipitation accumulates over several weeks up to
several months during the cold season (winter) and is released entirely in
the following spring and early summer. Glacier regimes result from perennial
snow and ice accumulation at elevations roughly beyond 3000 m a.s.l. Most
snow-dominated and glacier regimes are located in the Alps region (Fig. 3),
few of them are located south of the Alps,
which overall has a warmer climate and presents higher precipitation than the
other two regions.

Most Swiss discharge regimes show a strong seasonality (Weingartner and Aschwanden, 1992), illustrated in Fig. 2 for typical examples of the three regime main types; air temperature is shown here as a proxy for snow and evapotranspiration processes. The pluvial Goldach River (GOL) shows the typical summer low flow resulting from evapotranspiration; the Dischmabach shows a snow regime with high summer flows resulting from the release of snowmelt stored in the subsurface during the main snowmelt period (spring) and from residual snowmelt during summer. The Rhône River (RHG) with its 50 % glacier cover shows a glacier regime, with significant ice melt during summer, and with monthly discharge peaking for the same month as air temperature (July).

It is noteworthy that surface runoff processes definitely can play a certain role in extreme events in all regions of Switzerland (Bernet et al., 2017), but all hydrologic regimes are dominated by subsurface runoff processes, a precondition for the application of the modeling framework developed by Botter et al. (2007c).

Besides observed daily discharge, the model requires catchment-scale daily precipitation as input. Most of the previous applications of the models used precipitation from one or several meteorological stations as input (Botter et al., 2007c, a, 2013; Ceola et al., 2010; Basso et al., 2015; Schaefli et al., 2013), which is potentially limiting for the model performance since good area-averaged input estimates are critical. Recent progress in spaceborne precipitation observation, and in particular the Global Precipitation Measurement (GPM) mission, potentially offers an interesting new data source for area-averaged precipitation estimates, even in such complex terrain as the Swiss Alps (Gabella et al., 2017), with the drawback of covering only short historical periods. Here, we use the relatively new spatial precipitation data set of MeteoSwiss with a nominal resolution of 2.2 km and an effective resolution between 15 and 20 km and extending back to 1961 (MeteoSwiss, 2011a). This data set can be assumed to give relatively good estimates of area-averaged precipitation (Paschalis et al., 2014; Addor and Fischer, 2015), even in mountainous areas where there are only few meteorological stations.

Corresponding catchment-scale average precipitation time series per case study catchment are obtained by averaging the daily precipitation time series of all pixels contained in the catchment (a list of pixels per catchment is included in the Supplement). In addition, we also used the corresponding gridded temperature data set (MeteoSwiss, 2011b) to support the analysis of parameter seasonality. As for precipitation, the catchment-scale average temperature data set is obtained by averaging the daily time series of all pixels.

Before estimating rainfall frequency (*λ*_{p}) and average
rainfall depth on rain days
(*α*), the catchment-scale precipitation time series are
pre-processed to remove losses from interception. This step requires
information about land use. Of the retained 25 case study catchments, 22 are
part of what is called “hydrological study areas” and have an associated
extended data set, including land use (Aschwanden, 1996).
For the other catchments (i.e., the Areuse, Rhône-Gletsch and Venoge), land
use is obtained from the Swiss land use database (Federal Statistical Office, 2001).
Details about the land use estimation are available in the Supplement).

4 Results

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To gain further insights into the hydrological processes underlying the
different regimes, Fig. 4 shows the within-year
variability of the model parameters obtained by estimating the parameters in
forward mode for moving and overlapping 90-day windows. The precipitation
parameters *α* and *λ*_{p} do not show strong seasonal patterns,
except for a few catchments such as the Goldach River
(Fig. 4a). For snow and glacier regimes, the frequency of
discharge-producing events, *λ*, increases strongly at the beginning of
spring (Fig. 4b and c), which indicates the release of
water from snowmelt or ice melt.

The inverse of the linear recession coefficient $\mathit{\tau}={k}^{-\mathrm{1}}$ shows a
coherent annual cycle for all catchments, independent of the underlying
discharge regime (Fig. 5). This seasonal pattern with
consistently low *τ* values during summer for all catchments clearly
justifies the choice of a common summer season (June, July, August) for all
regimes. The amplitude of the annual cycle (the difference between high and
low *τ* values) is stronger for snow or glacier regimes, which reflects
the fact that in these regimes, parts of the catchment are effectively
dormant during the winter (Schaefli et al., 2013).

All estimated parameters for both forward and inverse estimations are
summarized in Table 2, together with the values of the
performance indicator *c*^{KS}. It can be noted that for 11
catchments (i.e., Rein da Sumvitg, Dischmabach, Alpbach, Grosstalbach,
Rhône à Gletsch, Massa, Verzasca, Riale di Calneggia, Krummbach,
Poschiavino and Ova da Cluozza), *λ* exceeds *λ*_{p},
contradicting the original description of the model
(Botter et al., 2007b), which states that the discharge-producing
frequency *λ* is smaller than the precipitation frequency
*λ*_{p}. Such an exceedance of *λ* over *λ*_{p}
should only happen in catchments or seasons with an additional source of
water (in addition to rainfall), which in the present case is snowmelt or ice
melt.

The exceedance of *λ* over *λ*_{p} increases with mean catchment
elevation (Fig. 6), the limit of
*λ*=*λ*_{p} being at around 1500 m a.s.l. This important result is
further discussed in Sect. 5.

The cdfs obtained from all estimated parameters are presented in Fig. 7 for the three example case studies. For the catchment with rainfall-driven discharges (GOL), it can be seen that the probabilities of occurrence of low flows are largely overestimated with forward estimation (Fig. 7a). This is a typical indication that the recession timescale is underestimated. The model values even exceed the envelopes that represent the natural variability of the discharges. In the presence of snow, the linear model in forward estimation mode tends to underestimate low flows, with satisfactory results for some cases, such as the Dischmabach (Fig. 7b).

Overall, there is a strong increasing trend of the linear model performance with mean catchment elevation (Fig. 9a). Despite this, the results of the linear model are not satisfactory for the forward estimation method for any of the regimes.

The inverse estimation of the model parameters improves the results
significantly, but the *c*^{KS} performance indicator shows
relatively high values and the curves are visually not accurate, especially
for pluvial regimes. This suggests that the model with a linear discharge
decay is overall not suitable for the studied catchments.

The results obtained from inverse parameter estimation for the nonlinear
model are very good (Fig. 8, Table 2),
and the nonlinear model outperforms the linear model for all catchments, both
in terms of the KS performance and in terms of the Akaike criterion (Table 2).
The relative model performance increase (as measured by
*r*^{AIC}) shows furthermore a strong inverse trend with mean
catchment elevation (Fig. 10), which results from the
increasing performance of the linear model with increasing elevation (Fig. 9b).

It is noteworthy that the two catchments for which the performance increase in the nonlinear model over the linear models exceeds 20 % are the two catchments that have a strongly karst-influenced regime (Scheulte at Vicques and Venoge at Ecublens).

As for the linear model, the forward estimation mode gives worse results
than the inverse estimation mode. For some catchments (i.e., Murg-Wängi,
Gürbe, Sense, Ilfis, and Grosstalbach), the forward estimation mode gives
nevertheless very good results with *c*^{KS} below 0.1. In general,
for the catchments where the discrepancies between modeled and observed cdfs
are due to an underestimation of *τ*, the nonlinear model yields a
significant improvement. For catchments where the recession timescale is
overestimated with the linear model, the nonlinear model in forward mode
leads to a performance decrease.

5 Discussion

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Our results show that analytical modeling framework for streamflow distributions proposed by Botter et al. (2007c) performs well for the 25 Swiss catchments across all studied discharge regimes. A detailed comparison between the performance of the linear and the nonlinear models considering the optimized parameters obtained from the inverse approach shows that the results for the nonlinear model are always better than for the linear model. This underlines that the nonlinear recession is better suited for the hydrological conditions of all studied catchments, which is in line with previous results (Ceola et al., 2010; Basso et al., 2015).

In forward estimation mode, the linear model outperforms the nonlinear model for catchments with summer high flows; the nonlinear model outperforms the linear model for catchments with rainfall-driven regimes (i.e., summer low flows). This results from the fact that for regimes with summer high flow, the linear model overestimates the recession timescale (resulting in a underestimation of the discharge variance). For regimes with summer low flow, the linear model in exchange underestimates the recession timescale. Given that the nonlinear model yields longer recessions, the nonlinear model shows accordingly a better performance for regimes with summer low flow.

The comparison between the forward and inverse estimation methods shows a
clear underestimation of *k*_{n} for most of the catchments, which was already
discussed by Dralle et al. (2015) and which is in line with previous work that
tried to improve the results of the model in forward estimation mode, for the
linear and the nonlinear formulation
(Ceola et al., 2010; Basso et al., 2015). There is clearly a need to
further improve the methods to estimate the recession parameters. Our results
pinpoint that a key here might be the detailed investigation of recession
analysis methods along elevational gradients and related hydrologic regimes.

Overall, good model performance in many different catchments with
different regimes indicates that the modeling framework is suitable for the
prediction of FDCs in Switzerland. A more detailed temporal model
validation (e.g., with a split sample test; Klemeš, 1986) is
not possible for this framework since the model parameters are obtained
directly from observed data for each time period (i.e., they vary from period
to period). The obtained model performances are comparable to the results
obtained in previous studies, e.g., in the work of
Ceola et al. (2010). For different case studies in
Italy and the US, they obtained *c*^{KS} values varying between 0.030 and 0.409
for the nonlinear model using different methods of forward estimation, and
*c*^{KS} values between 0.021 to 0.051 for inverse estimation.
For the linear model, Ceola et al. (2010) obtained *c*^{KS}
values between 0.054 and 0.567.
Basso et al. (2015) and Doulatyari et al. (2017) studied some
case studies that are included in the present paper (Sitter at Appenzell and
Murg at Wängi).

Recomputing their results with their model parameters yields slightly
different *c*^{KS} values for the nonlinear model for the Sitter
(0.12 compared to our 0.19) and for the Murg (0.05 to 0.06 compared to our
0.06). These differences are small and can be explained by different data
periods and by the methodological choices in the calculation of parameters.

The most remarkable result of the presented analysis is the fact that the
modeling framework is applicable in its original formulation to catchments
where summer flow is influenced by snow processes. The additional source of
water from snow or ice melt is accommodated by increasing the frequency
*λ* of discharge-producing events. This is in line with a common
assumption in catchment-scale precipitation–runoff modeling
(e.g., Schaefli et al., 2005), which is that runoff from snowmelt
can be modeled with exactly the same functional relationships as for
rainfall, by simply feeding so-called equivalent precipitation (sum of
rainfall and simulated snowmelt) into the runoff-generation module.

Furthermore, the increase in the discharge-producing frequency to account for snow or
ice melt is also coherent with the original description of the
analytic modeling framework, which incorporates losses as a decrease in the
discharge-producing frequency. This type of behavior can be identified in
previous studies. For the Sitter at
Appenzell, Basso et al. (2015) obtained *λ* values that are close to the precipitation frequency
*λ*_{p} during spring; for the Thur at Jonschwil they obtained
*λ*=*λ*_{p} for spring. Both catchments have a mean elevation above
1000 m a.s.l., which suggests the presence of snow processes. Later on,
Doulatyari et al. (2017) discussed that snow accumulation and melt could
be affecting the streamflow pdf estimation for the Sitter at Appenzell,
without, however, exploring the issue further.

As can be seen in Fig. 6, the switch from
*λ*<*λ*_{p} to *λ*_{p} to *λ*>*λ*_{p} is located at
around 1500 m a.s.l. This corresponds to a relatively low mean catchment
elevation; for this mean elevation, it can a priori not be assumed that
significant snowmelt continues throughout the summer. In fact, for most
snow-influenced catchments, the majority of snowmelt happens during spring.
Summer flows are nevertheless directly influenced by spring snowmelt since
the summer discharge results from a continuous release of melt water stored
in the catchment during the preceding snowmelt period. For high elevation
catchments, the exceedance of *λ* over *λ*_{p} is directly related
to significant snowmelt and ice melt inputs throughout the summer.

It should be kept in mind here that for the present study, *λ* is
estimated directly from the relationship between discharge and precipitation (see
Sect. 2.2 and Eq. 7). The question of how to estimate this parameter directly from
catchment characteristics based on long-term snow cover statistics and data
on glacier cover remains to be answered in future work.

Besides the important result that the model is applicable to snow-influenced catchments, additional insights can be obtained from the highlighted model performance trends with mean catchment elevation (Figs. 9 and 10). These performance trends are explained by the evolution of the regimes with mean catchment elevation, from rainfall-dominated (pluvial) regimes with summer low flow to snowfall-influenced (nival and glacier) regimes with summer high flow. This result suggests that mean catchment elevation is a good proxy for regime shifts, despite the fact that many other catchment characteristics vary strongly across the set of studied catchments (area, hypsometric curve, land use, etc.). Given the strong link between mean catchment elevation, mean catchment air temperature and snow accumulation, this opens interesting perspectives for parameter regionalization.

6 Conclusions

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This application of the analytic framework of Botter et al. (2007c) to estimate summer streamflow probability distributions for 25 Swiss catchments shows that this framework performs well without any further methodological adjustments across a wide range of discharge regimes, including rainfall-driven regimes with summer low flows, but also regimes with snowmelt- and glacier-melt-influenced summer high flows. Given that the original framework was developed for purely rainfall-driven regimes, this result is unexpected. For snow-influenced catchments, the model has been shown here to accommodate the additional source of water from snowmelt by a relative increase in the discharge-producing frequency, which is coherent with the underlying analytic framework.

The detailed comparison between the performance of the linear and the nonlinear model formulation shows that the description of Swiss summer flows strongly benefits from using a nonlinear storage–discharge relationship, in particular for catchments with summer low flow and for the karst catchments. In general, the linear model performance increases for increasing total summer flows or, equivalently, for catchments with higher mean elevation. Future work will focus on improving the model parameter estimation directly from observed data (without parameter optimization), which is a precondition for parameter regionalization. Better insights into the physical drivers of the different parameters will also open new potential for extending the model framework to all four seasons for all Swiss streamflow regimes.

Data availability

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Data availability.

The meteorological data used are not currently freely available; they require a license from MeteoSwiss. The discharge data are available upon request from the Swiss Federal Office for the Environment at https://www.hydrodaten.admin.ch/en/ (last access: 15 December 2017, FOEN, 2017). The basin boundaries used, obtained from the Swiss Federal Office for the Environment, are available in the Supplement as vector files.

Supplement

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Supplement.

The supplement related to this article is available online at: https://doi.org/10.5194/hess-22-2377-2018-supplement.

Competing interests

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Competing interests.

The authors declare that they have no conflict of interest.

Acknowledgements

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Acknowledgements.

The work of the first author is funded by the Portuguese Science and
Technology Foundation (FCT), grant no. PD/BD/52663/2014. The work of
Bettina Schaefli is funded by the Swiss National Science Foundation (SNSF), grant
no. PP00P2_157611. We thank the editor, Fabrizio Fenicia, and two anonymous
reviewers for their detailed comments on an earlier version of this
manuscript.

Edited by: Fabrizio Fenicia

Reviewed by: two anonymous referees

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Short summary

This paper assesses the performance of an analytical modeling framework for probability distributions for summer streamflow of 25 Swiss catchments that present a wide range of hydroclimatic regimes, including snow- and icemelt-influenced streamflows. Two versions of the model were tested: linear and nonlinear. The results show that the model performs well for summer discharges under all analyzed regimes and that model performance varies with mean catchment elevation.

This paper assesses the performance of an analytical modeling framework for probability...

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