2015
DOI: 10.1080/19942060.2015.1004811
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A cost-effective FE method for 2D Navier–Stokes equations

Abstract: A cost-effective approach to the solution of 2D Navier-Stokes equations for incompressible fluid flow problems is presented. The aim is to reach a good compromise between numerical properties and computational efficiency. In order to achieve the set goal, the nonlinear convective terms are approximated by means of characteristics and spatial approximations of equal order are performed by polynomials of degree two. In this way, the computational kernels are reduced to elliptic ones for which solution very effic… Show more

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Cited by 6 publications
(3 citation statements)
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“…In table 1 we compare the results obtained from the suggested method with the methods KRDRM and KPIM of velocity 𝑢 along the vertical line and 𝑣 velocity along the horizontal line through the geometric center of the square cavity, the findings demonstrate that these values are identical with values stated in KRDRM and KPIM for various values of Renolds numbers at 𝑡 = 0.1 𝑎𝑛𝑑 𝑀𝑎 = 0.01 ,was q-HALPM solutions from two iterations .Table 2 represented the results 𝑢 𝑎𝑛𝑑 𝑣 that are obtained from q-HALPM with KRDRM, KPIM and finite volume method in Ref [9]. The 𝐿 ∞ − 𝑒𝑟𝑟𝑜𝑟𝑠 shows in Table 3 for the stream function 𝜓 and the vorticity 𝜔 by using the current method and comparted with these provided methods in [1] and [9] and rational fourth-order compact finite difference method in [33] , for three different values of Reynolds numbers 𝑅𝑒 = 10,100 𝑎𝑛𝑑1000 𝑎𝑡 𝑀𝑎 = 0.001, We see that the number of grid points has no bear on the estimated errors, which are small for all Reynolds number values. The analytical approximate solution produced by 𝑣(0.9375; 0.5) −0.15380859374 −0.1429446548 −0.1429451057…”
Section: -Results and Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…In table 1 we compare the results obtained from the suggested method with the methods KRDRM and KPIM of velocity 𝑢 along the vertical line and 𝑣 velocity along the horizontal line through the geometric center of the square cavity, the findings demonstrate that these values are identical with values stated in KRDRM and KPIM for various values of Renolds numbers at 𝑡 = 0.1 𝑎𝑛𝑑 𝑀𝑎 = 0.01 ,was q-HALPM solutions from two iterations .Table 2 represented the results 𝑢 𝑎𝑛𝑑 𝑣 that are obtained from q-HALPM with KRDRM, KPIM and finite volume method in Ref [9]. The 𝐿 ∞ − 𝑒𝑟𝑟𝑜𝑟𝑠 shows in Table 3 for the stream function 𝜓 and the vorticity 𝜔 by using the current method and comparted with these provided methods in [1] and [9] and rational fourth-order compact finite difference method in [33] , for three different values of Reynolds numbers 𝑅𝑒 = 10,100 𝑎𝑛𝑑1000 𝑎𝑡 𝑀𝑎 = 0.001, We see that the number of grid points has no bear on the estimated errors, which are small for all Reynolds number values. The analytical approximate solution produced by 𝑣(0.9375; 0.5) −0.15380859374 −0.1429446548 −0.1429451057…”
Section: -Results and Discussionmentioning
confidence: 99%
“…Now, before we start applying the q-HALPM on KRLNS equation taking the initial conditions of 𝑢, 𝑣, 𝑃 as [31][32][33];…”
Section: Deffinition22mentioning
confidence: 99%
“…Since two decades ago, researchers have done lots of work on dynamics of particles' freefalling in fluids both experimentally and numerically (Ardekani, Dabiri, & Rangel, 2008;Feng & Michaelides, 2004;Goyal & Derksen, 2012;Hu, 1996;Huang, Hu, & Joseph, 1998;Pu, Shao, Huang, & Hussain, 2013). Among the numerical methods, finite element method (FEM) (Jotsa & Pennati, 2015;Liu & Quek, 2013), finite difference method (FDM), finite volume method (FVM), and even meshfree methods (Liu, 2009;Pu et al, 2013) are most widely used. Hu, Joseph, and Crochet (1992) used FEM to model the Navier-Stokes equations for liquid and the Newton's equations of motion for solids.…”
Section: Introductionmentioning
confidence: 99%