1983
DOI: 10.1016/0307-904x(83)90118-x
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Finite Elements and characteristics for some parabolic-hyperbolic problems

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Cited by 74 publications
(28 citation statements)
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“…n, = 0 are given as the boundary conditions. Strp 7: Repeat steps 3-6 using the working equation (20) instead of equation (24) and obtain the values of water depth at all nodal points. The only boundary conditions prescribed in this step are the water depths, as a function of time, at the down-stream side of the flow domain.…”
Section: Solution Algorithmmentioning
confidence: 99%
“…n, = 0 are given as the boundary conditions. Strp 7: Repeat steps 3-6 using the working equation (20) instead of equation (24) and obtain the values of water depth at all nodal points. The only boundary conditions prescribed in this step are the water depths, as a function of time, at the down-stream side of the flow domain.…”
Section: Solution Algorithmmentioning
confidence: 99%
“…Then the Lagrangian total derivative is approximated thanks to some divided difference operator. These methods have largely proven their efficiency (see for example [1,2,6,15,16] Let T > 0. We consider a (not necessarily uniform) subdivision of (0, T ): 0 = T 0 < T 1 < ... < T Q−1 < T Q = T .…”
Section: Introductionmentioning
confidence: 99%
“…In this problem, A is an artificial velocity and V • A is not necessary nuil so we will have to take it into consideration and compute it. Next, we shall follow the notation and ideas presented in [4].…”
Section: Numerical Analysis Of the Radially Symmetrical Case In 2dmentioning
confidence: 99%
“…(10), weopt for using a scheme which combines the method of characteristics and the reformulation of the convection term in (10) in terms of the total derivative with the finite element one (see [4,8] and references therein). We shall assume that the variables satisfy some regularity requirements that allow us to develop the numerical scheme.…”
Section: Numerical Analysis Of the Radially Symmetrical Case In 2dmentioning
confidence: 99%
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