A critical assessment of the performance of standard 2D flood models based on results of 3D URANS simulations D.V. Horna Munoz IIHR-Hydroscience and Engineering, The University of Iowa, Iowa City, Iowa, United States of America ABSTRACT: Evaluating the accuracy of 2D depth-averaged solvers to predict flood propagation in natural environments is one of the most important challenges to mitigate floods. This paper discusses the performance of SRH-2D, a standard 2D flood propagation solver in terms of predicted flood extent and depth-averaged velocity profiles in a complex bathymetry river reach for high flow conditions. The accuracy of the 2D solver is mainly evaluated based on comparison with results obtained using a 3D URANS two-phase flow model developed using the commercial software STAR-CCM+. The 2D model performance is evaluated for a steadystate test case. The domain contains a 7-km reach of the Iowa River near Iowa City and 2 river dams. Even though the SRH-2D depth-averaged velocities show the same pattern as the 3D depth-averaged results, the 2D model tends to underpredict the location and magnitude of the peak unit discharge inside the channel, especially in the regions where 3D effects are significant. 1 INTRODUCTION The standard practice for simulating realistic flood events is the application of numerical models based on solving the 1-D, 2-D or hybrid 1-D/2-D shallow water (Saint-Venant) equations. The use of 1-D codes is highly popular since they are able to compute flood events in natural environments in large domains in a relatively short amount of time and using readily available computing resources. 1-D codes assume the flow is essentially unidirectional making them incapable of simulating lateral diffusion of flood waves into the floodplain (Hunter, et al 2007). 2-D codes overcome these limitations by solving the 2-D Saint Venant equations, which are obtained by depth-averaging the Navier-Stokes equations. The main limitations of the 2-D Saint Venant equations arise from the derivation of the equations, in which hydrostatic pressure distribution is assumed over the vertical direction. It is because of these limitations that 2-D codes are unable to accurately predict mean flow and turbulence in regions where the flow is highly 3D and nonisotropic (flows with separation, flow around hydraulic structures, river confluences, etc.). It is well documented that the flow field increases its level of three dimensionality during unsteady events such as floods, especially in regions of high stream curvature, around hydraulic structures and in the transition region be- tween main channel and floodplain. These flow complexities make a strong case for the use of a 3-D nonhydrostatic Navier Stokes model with deformable free-surface capabilities to simulate unsteady flood wave propagation in the domain. Such models should be able to offer a better representation of the mean flow field across the domain. By simulating exactly the same test case using the 3-D and the 2-D model, one can get a better idea about the accuracy of the latter model. This is important, given the lack of extended validation data for flood predictions. In the present paper, we report a case study in which the flood extent and depth-averaged velocity profiles were obtained in a 6-km reach of the Iowa River near Iowa City (Iowa, United States of America) for steady state under high flow conditions. The reach contains two dams (Fig. 1). The bathymetry and topography information were provided by the Iowa Flood Center. Results obtained using SRH-2D, a standard 2-D depth-averaged shallow flow solver, are compared to those obtained with STAR-CCM+, a 3D non-hydrostatic viscous solver using the k-ε turbulence model and a deformable free-surface module based on the Volume-of-Fluid (VOF) method. A mesh with 6 million cells was used in 3D simulation. SRH-2D solves the full 2-D Shallow Water equations with a parabolic turbulence model. Roughness parametrization was accounted by specifying regions with different values of Manning’s coefficient across the domain. 3 CONCLUSIONS AND FUTURE WORK The results reported in this paper suggests that the predictive capabilities of 2D solvers used to model flood propagation can decay significantly in regions where 3D effects are important. Future research plans include performing an unsteady simulation in the same river reach to assess the performance of the 2D model during a fast extreme flood event. Figure 1. Close-up view showing the start of computational domain (1’-1’), the end of the computational domain (2’-2’), the location of the first river dam (2-2) and the location of the second river dam (3-3). 2 RESULTS Based on comparison with USGS gage at the only location where stage was measured, the results obtained with the calibrated SRH-2D model overestimate the free-surface elevation by approximately 1 ft (30 cm) while STAR-CCM+ underestimate the measured data. It is important to mention that while SRH-2D had to be calibrated for low and high flow conditions, STAR-CCM+ results were obtained with no calibration. At steady state, the difference in flood extent area is approximately 21% with respect to the results obtained with STAR-CCM+. Flood extents for STAR-CCM+ (3D) and SRH-2D (2D) are shown in Figure 2 and 3 respectively. Qualitatively, there is little difference between the flood extents. The most noticeable difference is observed near the area between cross-sections 1 and 2, in which SRH-2D inundates a significant amount of area more compared to STAR-CCM+. Areas close to cross-sections 7 and 8 also show a slight difference between the 2 solutions. The full paper contains a detailed comparison between the unit-discharge profiles in representative cross-sections between the 2D and 3D models. The comparison will show that several regions are present where fairly significant differences occur between the two models. They generally happen in regions where the degree of flow three-dimensionality is high (e.g., regions of high channel curvature, regions containing large-scale deformations at the bed). Figure 2. Aerial view of flood extent for results obtained with STAR-CCM+ Figure 3. Aerial view of flood extent for results obtained with SRH-2D REFERENCES Frank, E. A., Ostan, A., Coccato, M., and Stelling, G. 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