2014
DOI: 10.1002/2013jc009604
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Uncertainty in hurricane surge simulation due to land cover specification

Abstract: Hurricane storm surge is one of the most costly natural hazards in the United States. Numerical modeling to predict and estimate hurricane surge flooding is currently widely used for research, planning, decision making, and emergency response. Land cover plays an important role in hurricane surge numerical modeling because of its impacts on the forcing (changes in wind momentum transfer to water column) and dissipation (bottom friction) mechanisms of storm surge. In this study, the hydrodynamic model ADCIRC wa… Show more

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Cited by 32 publications
(27 citation statements)
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“…Manning's n coefficient of 0.03 and 0.17 might be associated with pasture or grassland and mixed forest [31], therefore, the model is very sensitive to the land cover classification. It might confirm what Ferreira et al (2014) [43] demonstrated, and an incorrect land cover choice may lead to error in surge of 7.0%. Resio and Westerink (2008) [9] discussed that an increased frictional resistance slows the rate the flood wave moves inland.…”
Section: Storm Surge In Overland Areassupporting
confidence: 56%
“…Manning's n coefficient of 0.03 and 0.17 might be associated with pasture or grassland and mixed forest [31], therefore, the model is very sensitive to the land cover classification. It might confirm what Ferreira et al (2014) [43] demonstrated, and an incorrect land cover choice may lead to error in surge of 7.0%. Resio and Westerink (2008) [9] discussed that an increased frictional resistance slows the rate the flood wave moves inland.…”
Section: Storm Surge In Overland Areassupporting
confidence: 56%
“…ADCIRC is a finite‐element hydrodynamic model that generates water levels and current velocities, and is widely used for storm surge modelling in the east coast of United States and Gulf of Mexico (e.g. Ferreira et al , ). We used the 2D, depth‐integrated version of ADCIRC (Luettich and Westerink, ) that solves the vertically integrated generalised wave continuity equation (GWCE) and the momentum equations (Eqns and , respectively): h t + h () true U h = 0 true U t + () U . h true U = prefix− g h () ζ + p (), x y g ρ + f true k × true U + true τ normals h ρ true τ normalb h ρ where h is bathymetric depth, t is the time, ζ is surge elevation above MSL, true U is depth‐averaged horizontal velocity vector, p is barometric pressure, f is the Coriolis force coefficient, true k is a vertical unit vector, τ s is the free surface shear stress, τ b is the bottom shear stress, ρ is the water density and g is gravitational acceleration.…”
Section: Methodsmentioning
confidence: 99%
“…Bottom friction is parameterized in ADCIRC using a quadratic bottom stress, where the bottom drag coefficient is dependent on the Manning's n coefficient and depth at each mesh node (Kerr, Martyr, et al). Correct nearshore and overland frictional representation is critical to accurately simulating peak coastal water levels and inundation (Ferreira et al, ). A Manning's n of 0.025 and 0.028 was used for the Atlantic Ocean and the Caribbean Sea, respectively.…”
Section: Model Data and Experimental Descriptionmentioning
confidence: 99%