2004
DOI: 10.1016/j.ijthermalsci.2003.11.002
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Application to natural convection enclosed flows of a lattice Boltzmann BGK model coupled with a general purpose thermal boundary condition

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Cited by 154 publications
(58 citation statements)
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“…This term, can be added to rp to obtain an effective pressure gradient rp 0 = r(p + 1/2w 2 ), which increases the pressure near the wall. A similar inclusion of gradients of scalar potentials has been reported in the context of buoyancy-driven flows (de Vahl Davis 1983;D'Orazio et al 2004) and thermomagnetic convection (Mukhopadhyay et al 2005) in enclosures. The pressure can be obtained form the relation p 0 ¼ 1 3 qc 2 : At all the four walls no-slip boundary condition is applied as proposed by Zou and He (1997).…”
Section: And 'supporting
confidence: 61%
“…This term, can be added to rp to obtain an effective pressure gradient rp 0 = r(p + 1/2w 2 ), which increases the pressure near the wall. A similar inclusion of gradients of scalar potentials has been reported in the context of buoyancy-driven flows (de Vahl Davis 1983;D'Orazio et al 2004) and thermomagnetic convection (Mukhopadhyay et al 2005) in enclosures. The pressure can be obtained form the relation p 0 ¼ 1 3 qc 2 : At all the four walls no-slip boundary condition is applied as proposed by Zou and He (1997).…”
Section: And 'supporting
confidence: 61%
“…By performing Taylor-series expansion analysis and conservation laws, it can be proven that Equations (24)- (26) in the predictor step can recover corresponding macroscopic Equations (17)- (19) with the second-order of accuracy both in time and in space. However, in the corrector step, it can be shown that when recovering macroscopic Equations (21) and (22), Equations (28) and (29) maintain the second-order of accuracy in space, but present a Euler scheme in time marching, which is only in the first-order of Appl.…”
Section: Simplified Thermal Lattice Boltzmann Methods (Stlbm)mentioning
confidence: 99%
“…As with the single-phase system, this model has been validated over many years by repeated analyses and comparisons with analytical and experimental results [14,16,18,44,45]. It has been successfully applied to a variety of thermal flow problems including natural convection [14,18,44,[46][47][48][49][50], turbulent convection [51][52][53][54], thermal channel flows [14,40,55,56] and more complex systems involving multiple phases and phase change [57][58][59][60][61][62][63][64][65].…”
Section: Thermohydrodynamicsmentioning
confidence: 99%