1997
DOI: 10.1016/s0045-7825(96)01053-5
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Temporal, spatial and thermal features of 3-D Rayleigh-Bénard convection by a least-squares finite element method

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Cited by 23 publications
(20 citation statements)
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“…[11], [12], [15], [18], [87], [91]- [94], [96], [99], [112], and [113]. Exceptions include [13] and [14] which consider velocity gradient methods, and [92] where a stress-based method is discussed.…”
Section: H −1 Least-squares Methodsmentioning
confidence: 99%
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“…[11], [12], [15], [18], [87], [91]- [94], [96], [99], [112], and [113]. Exceptions include [13] and [14] which consider velocity gradient methods, and [92] where a stress-based method is discussed.…”
Section: H −1 Least-squares Methodsmentioning
confidence: 99%
“…The limited space did not allow us to consider many other important areas, such as hyperbolic problems, time dependent problems, and time-space leastsquares. For further details on such applications, we refer interested readers to [4], [9], [39], [40], [41], [62], [63], [88], [89], and [110]- [113], among others.…”
Section: Restricted Least-squares Methodsmentioning
confidence: 99%
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“…After these coefficients are determined, the Galerkin series (22) satisfy all the linear homogeneous boundary conditions analytically (for details see [4]). Note also that the projection of the pressure gradient on the divergent-free basis (23), (24) is analytically zero [4], which means that the Galerkin procedure eliminates the perturbation of pressure from (14). Therefore, we do not need an approximation of the pressure.…”
Section: Methodsmentioning
confidence: 99%