1982
DOI: 10.1002/fld.1650020404
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Finite element, stream function–vorticity solution of steady laminar natural convection

Abstract: SUMMARYStream function-vorticity finite element solution of two-dimensional incompressible viscous flow and natural convection is considered. Steady state solutions of the natural convection problem have been obtained for a wide range of the two independent parameters. Use of boundary vorticity formulae or iterative satisfaction of the no-slip boundary condition is avoided by application of the finite element discretization and a displacement of the appropriate discrete equations. Solution is obtained by Newto… Show more

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Cited by 29 publications
(7 citation statements)
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“…[14]. See [7,12] for the case of the biharmonic equation and [2,1,5,18,25] for the steady Navier-Stokes equation. The main contribution of this paper is an efficient time stepping procedure of (1.5) which will be described in Section 2.…”
Section: Introductionmentioning
confidence: 99%
“…[14]. See [7,12] for the case of the biharmonic equation and [2,1,5,18,25] for the steady Navier-Stokes equation. The main contribution of this paper is an efficient time stepping procedure of (1.5) which will be described in Section 2.…”
Section: Introductionmentioning
confidence: 99%
“…To solve this problem in the same form as given by others, 25 Results are presented in terms of the Rayleigh number, which is Ra = GrPr. All results are given for Pr =0.71.…”
Section: Natural Convection Problemmentioning
confidence: 99%
“…In this paper the theoretical aspects is explained only for natural convection but in the illustrations both advection and natural convection problems were discussed. If the internal heating by viscous dissipation is neglected, :t/L chosen as u* and the Rayleigh and Prandtl numbers employed as dimensionless groups, eqns (12) and (13) may be rewritten as:…”
Section: The Density Satisfies An Equation Of State Of the Form P = Pmentioning
confidence: 99%