Most methods for directly measuring the discharge of a water stream are time-consuming and expensive. Therefore, indirect methods for measuring the discharge are usually applied. A popular method for inferring discharge is to fit a model that describes the relationship between the discharge and the water level, also referred to as water elevation. Such a model is called a discharge rating curve, and one widely used in hydrology is the power-law rating curve, given by \(Q(h)=a(h-c)^b\), where \(Q(h)\) is the discharge, \(h\) is the water elevation, and \(a\), \(b\) and \(c\) are constants. However, the power-law rating curve is not always able to adequately describe the relationship between discharge and water elevation. Hrafnkelsson et al. (2022) proposed a novel extension to the power-law rating curve referred to as the generalized power-law rating curve. Its form is \(Q(h)=a(h-c)^{f(h)}\), where the power-law exponent, \(f(h)\), is a function of water elevation. This generalization allows the water stream’s cross-sectional geometry to affect the power-law exponent, lending more flexibility to the rating curve to adequately describe the relationship between discharge and water elevation.

The power-law model is commonly assumed in hydraulic practice to fit rating curves, and as mention above, its form is

\[Q(h) = a(h-c)^{b}\] (1)

where \(Q\), \(h\), \(a\), \(b\) and \(c\) are as before, see e.g., Venetis (1970), Clarke (1999) and Clarke et al. (2000). The second type of rating curve is the generalized power-law rating curve. Its construction is based on the hydraulics of open channel flow given by the formulas of Chézy and Manning which are of the form

\[Q = KR^{x}AS^{1/2}\] (2)

where \(K\) and \(x\) are constants; \(A\) is the area of the cross section; \(S\) is the slope of the channel; and \(R\) is the hydraulic radius, given by \(R = A/P\), where \(P\) is the wetted perimeter. According to Chézy \(x = 1/2\), while Manning claimed that \(x = 2/3\) (Chow, 1959). The form of the generalized power-law rating curve is

\[Q = a(h − c)^{f(h)}\] (3)

where \(a\) and \(c\) are constants; and \(f(h)\) is a function of \(h\), referred to as the power-law exponent. The relationship between (2) and (3) can be found by equating these two equations. In particular, the form of \(f(h)\) can be derived, namely,

\[f(h) = \frac{(x+1)\{ \log A(h) - \log A(1) \} - x \{ \log P(h) - \log P(1) \}}{\log h}\] (4)

Thus, \(f(h)\) is a function of the constant \(x\), the cross-sectional area \(A\), and the wetted perimeter \(P\). A Bayesian approach is proposed for estimating the parameters of the power-law model and the generalized power-law model. Bayesian inference requires specification of prior densities for unknown parameters and unknown quantities, along with a full probabilistic specification of the observed data. The goal of Bayesian inference is to obtain the posterior density of the model parameters, and then interrogate the posterior by calculating summary statistics, such as the posterior mean and the 95% posterior intervals. Analytical formulas for these summary statistics are intractable in most cases and thus they are computed by generating samples from the posterior density using Markov chain Monte Carlo simulation. The Bayesian power-law model is presented on a logarithmic scale as,

\[\log(Q_i) = \log(a) + b \log(h_i -c) + \epsilon_i, \quad i = 1,...,n,\] (5)

where \(\epsilon_i\) follows a normal distribution with mean zero and variance \(\sigma_{\epsilon}^2\), \(n\) is the number of paired observations, and \(a\), \(b\) and \(c\) are as before. The Bayesian inference scheme implemented for the power-law model is standard, however, for efficient posterior simulation, first, samples are obtained from the joint marginal posterior density of \((c, \sigma_{\epsilon}^2)\), then samples are obtained from the conditional posterior density of \((\log(a), b)\) conditional on \((c, \sigma_{\epsilon}^2)\). The Bayesian generalized power-law model is presented as a Bayesian hierarchical model. The function \(f(h)\) is modeled at the latent level as \(b\) plus a mean zero continuous stochastic process \(\beta(h)\), which is assumed to be twice mean-square differentiable. The model is presented on a logarithmic scale as,

\[\log (Q_i) = \log (a) + (b + \beta(h_i)) \log(h_i -c) + \varepsilon_i, \quad i = 1,...,n,\] (6)

where \(\epsilon_i\) follows a normal distribution with mean zero and variance \(\sigma_{\epsilon}^2(h_i)\) that can vary with water elevation. Here the parameters \(a\), \(b\) and \(c\) play a similar role as in the Bayesian power-law model. The stochastic process \(\beta(h)\) is assumed a priori to be a Gaussian process governed by a Matérn covariance function with smoothness parameter \(\nu = 2.5\), see Matérn (1960). This model is constrained by setting \(b=1.835\). An efficient posterior simulation is achieved by sampling from the joint posterior density of the hyperparameters of the model, and then sampling from the conditional density of the latent parameters given the hyperparameters.

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Clarke, R., Mendiondo, E., Brusa L. (2000). *Uncertainties in mean
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Hrafnkelsson, B., Sigurdarson, H., and Gardarsson, S. M. (2022).
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