1999
DOI: 10.1002/(sici)1097-0363(19990228)29:4<397::aid-fld793>3.0.co;2-n
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An operator splitting numerical scheme for thermal/isothermal incompressible viscous flows

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Cited by 12 publications
(12 citation statements)
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“…Figures 3 and 4 show the ows for Reynolds number Re = 1000 and Grashof numbers Gr = 10 2 and Gr = 10 6 in the unit square cavity on a mesh (h x ; h y ) = (1=120; 1=120), both with t = 0:01; the streamlines on the left are obtained with the contour values given by Ghia et al [15] whereas the isotherms on the right are 'default' ones. Both results agree with those in Reference [6]; they in turn were validated with the ones in Reference [14]. The validation from this work is reinforced by showing in Figure 5 the proÿles of the horizontal U and vertical V component of the velocity at x = 0:5 (left) and y = 0:5 (right), respectively, for Gr = 10 6 ÿxed and Re = 400, 1000, 3000, with their min-max values given in Table I.…”
Section: Mixed Convection Thermal Owssupporting
confidence: 93%
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“…Figures 3 and 4 show the ows for Reynolds number Re = 1000 and Grashof numbers Gr = 10 2 and Gr = 10 6 in the unit square cavity on a mesh (h x ; h y ) = (1=120; 1=120), both with t = 0:01; the streamlines on the left are obtained with the contour values given by Ghia et al [15] whereas the isotherms on the right are 'default' ones. Both results agree with those in Reference [6]; they in turn were validated with the ones in Reference [14]. The validation from this work is reinforced by showing in Figure 5 the proÿles of the horizontal U and vertical V component of the velocity at x = 0:5 (left) and y = 0:5 (right), respectively, for Gr = 10 6 ÿxed and Re = 400, 1000, 3000, with their min-max values given in Table I.…”
Section: Mixed Convection Thermal Owssupporting
confidence: 93%
“…Taking into account that the elliptic system (10), in addition to being non-linear, is of the non-potential (or transport) type, a ÿxed point iterative process is used for the solution. This process is similar to one applied previously to mixed convection problems in primitive variables [6]. A distinctive aspect here is that the iterative process is extended up to the boundary to handle the !…”
Section: Numerical Schemementioning
confidence: 99%
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“…The analysis concentrated mostly on the validation and physical correctness of the obtained solutions, although the numerical efficiency was also addressed. In the other publication (Bermudez and Nicolas, 1999), a fractional-time-step algorithm has been proposed for unsteady thermally-coupled flows. In this approach, the main time step is divided into three equal sub-steps.…”
Section: Introductionmentioning
confidence: 99%