1991
DOI: 10.1002/fld.1650120402
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An upwind finite element scheme for high‐Reynolds‐number flows

Abstract: SUMMARYA new upwind finite element scheme for the incompressible Navier-Stokes equations at high Reynolds number is presented. The idea of the upwind technique is based on the choice of upwind and downwind points. This scheme can approximate the convection term to third-order accuracy when these points are located at suitable positions. From the practical viewpoint of computation, the algorithm of the pressure Poisson equation procedure is adopted in the framework of the finite element method. Numerical result… Show more

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Cited by 41 publications
(22 citation statements)
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“…The fourth step is a hyperbolic problem for the scalar level-set function ~b. This problem is solved by using a upwinding scheme where the advection term is discretized using a third-order scheme [18,19,23]. That is, u -V~b at x ° is estimated using the known values of ~b at the five points X -2, X -l , X 0, X 1 , and X 2, which lie on the line that is parallel to u and passes through x °, u. V4>(x °) = lu(x°)l ~ rj4~(xJ) where ~i = IX i __ X0]/h.…”
Section: Remarksmentioning
confidence: 99%
“…The fourth step is a hyperbolic problem for the scalar level-set function ~b. This problem is solved by using a upwinding scheme where the advection term is discretized using a third-order scheme [18,19,23]. That is, u -V~b at x ° is estimated using the known values of ~b at the five points X -2, X -l , X 0, X 1 , and X 2, which lie on the line that is parallel to u and passes through x °, u. V4>(x °) = lu(x°)l ~ rj4~(xJ) where ~i = IX i __ X0]/h.…”
Section: Remarksmentioning
confidence: 99%
“…Yet another alternative is provided by Singh and Leal [29] who apply a third order upwind scheme of Tabata and Fujima [30], while special measures where taken to maintain a positive definite conformation tensor.…”
Section: Problem 1 (Mix)mentioning
confidence: 99%
“…Approximation (32) is not mass-conservative even if the definition is extended appropriately to V h ⊂ H 1 (Ω). (32) is extended to second-and third-order upwind approximations for high-Reynolds number flow problems [9], [19]. …”
Section: A1 the Upwind Element Choice Approximation [17]mentioning
confidence: 99%