2005
DOI: 10.1016/j.ocemod.2004.06.006
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An efficient Eulerian finite element method for the shallow water equations

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Cited by 102 publications
(56 citation statements)
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“…In the final numerical test, we solve the equatorial Rossby soliton analytically studied by Boyd [5], and used to validate numerical models in [12,17] among others. The rotational effect of the Earth is included through the Coriolis force.…”
Section: Solitary Rossby Wavementioning
confidence: 99%
“…In the final numerical test, we solve the equatorial Rossby soliton analytically studied by Boyd [5], and used to validate numerical models in [12,17] among others. The rotational effect of the Earth is included through the Coriolis force.…”
Section: Solitary Rossby Wavementioning
confidence: 99%
“…More recent mathematical and numerical analysis of finite element pairs for gravity and Rossby waves are provided in Le Roux et al (2007, , and . Hanert et al (2005) proposed to use the P NC 1 -P 1 pair, following Hua and Thomasset (1984). It appears that the P NC 1 -P 1 pair is a stable discretization, but its rate of convergence is suboptimal on unstructured grids (Bernard et al 2008b).…”
Section: Introductionmentioning
confidence: 99%
“…Earlier experiments with P NC 1 − P 1 code revealed problems with spatial noise and instability of the momentum advection when the discretisation is used as described by Hanert et al (2005). A modified implementation without upwinding terms was found to work well when paired with rather high viscous dissipation to remove small-scale noise in the velocity field.…”
Section: Momentum Advection Schemementioning
confidence: 93%
“…The main reason to choose finite elements is the computational mesh that can be adapted to cover basins with irregular bottom topography and coastlines. The spatial discretisation of TsunAWI is based on the finite element approach by Hanert et al (2005) with modifications like added viscous and bottom friction terms, corrected momentum advection terms, radiation boundary condition, and nodal lumping of mass matrix in the continuity equation. The basic principles of discretisation follow Hanert et al (2005) with linear conforming elements P 1 for sea surface height ζ and water depth h, and linear non-conforming elements P NC 1 for the velocity v. Thus, values for sea surface are computed at element nodes, while the velocity components are regarded at the edges.…”
Section: Finite Element Methodsmentioning
confidence: 99%