2022
DOI: 10.5194/gmd-2022-259
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LISFLOOD-FP 8.1: New GPU accelerated solvers for faster fluvial/pluvial flood simulations

Abstract: Abstract. The local inertial two-dimensional (2D) flow model on LISFLOOD-FP, so-called ACC uniform grid solver, has been widely used to support fast, computationally efficient fluvial/pluvial flood simulations. This paper describes new releases, on LISFLOOD-FP 8.1, for parallelised flood simulations on the graphical processing units (GPU) to boost efficiency of the existing parallelised ACC solver on the central processing units (CPU) and enhance it further by enabling a new non-uniform grid version. The non-u… Show more

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Cited by 4 publications
(10 citation statements)
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“…In the future, it would be interesting to extend this modeling approach to bigger watersheds to test the overall run time, even considering more HPC‐enabled solutions to enhance the computational efficiency (Caviedes‐Voullième et al., 2023; Morales‐Hernández et al., 2021; Sharifian et al., 2023).…”
Section: Discussionmentioning
confidence: 99%
“…In the future, it would be interesting to extend this modeling approach to bigger watersheds to test the overall run time, even considering more HPC‐enabled solutions to enhance the computational efficiency (Caviedes‐Voullième et al., 2023; Morales‐Hernández et al., 2021; Sharifian et al., 2023).…”
Section: Discussionmentioning
confidence: 99%
“…For probabilistic modeling of slowly propagating fluvial/pluvial floods over large catchments, a less complex (mathematically and numerically) physical solver may be more appropriate to expedite runtimes, such as the reduced acceleration solver on LISFLOOD‐FP (Beevers et al., 2020), which has a version for the GPU with grid‐resolution adaptivity to maximize runtime efficiency (Sharifian et al., 2023). Alternatively, physical solvers based on distributed hydrological modeling can be used for multi‐physics modeling such as to incorporate the feedbacks between groundwater and land surface processes (for example, Baroni et al., 2019).…”
Section: Limitations and General Applicabilitymentioning
confidence: 99%
“…Therefore, a uniform inflow discharge random variable, Q ( t , ξ Q ), follows: Q()t,ξQ=trueQ(t)+ξQ0.25emσQ(t) $Q\left(t,{\xi }_{Q}\right)=\overline{Q}(t)+{\xi }_{Q}\,{\sigma }_{Q}(t)$ where ξ Q is a random variable taking values in [−1,+1] and σQ(t)=0.08trueQ(t) ${\sigma }_{Q}(t)=0.08\overline{Q}(t)$ is the range of variation with respect to the mean trueQ(t) $\overline{Q}(t)$. In flood modeling, a number of P mean inflow discharges, trueQ1(t) $\overline{{Q}_{1}}(t)$, …, trueQP(t) $\overline{{Q}_{P}}(t)$ ( P > 1), can be given (Kesserwani & Sharifian, 2023; Sharifian et al., 2023). In this case, the variation in each of Q1()t,ξQ1 ${Q}_{1}\left(t,{\xi }_{{Q}_{1}}\right)$, …, QP()t,ξQP ${Q}_{P}\left(t,{\xi }_{{Q}_{P}}\right)$ follows Equation , assuming that ξQ1 ${\xi }_{{Q}_{1}}$, …, ξQP ${\xi }_{{Q}_{P}}$ are not intercorrelated (Neal et al., 2013), leading to an uncertainty space dimension of D = P .…”
Section: Uq Analysis Frameworkmentioning
confidence: 99%
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“…However, mathematical rigorous a priori or a posteriori error estimates for nonlinear systems of Shallow Water Equations (SWEs) are generally unavailable (Gerhard & Müller, 2014). In this paper, multiresolution analysis of underlying topography based on wavelet theory is implemented to construct a hierarchical quadtree grid (Caviedes‐Voullième et al., 2020; Gerhard et al., 2015; Kesserwani & Sharifian, 2023; Sharifian et al., 2023), which facilitates error control as a key aspect as opposed to traditional methods for AMR (Gerhard et al., 2015; Kesserwani et al., 2019).…”
Section: Introductionmentioning
confidence: 99%