2007
DOI: 10.1016/j.enconman.2006.11.013
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Direct simulation of natural convection in square porous enclosure

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Cited by 23 publications
(21 citation statements)
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“…(17), N minÀv is not affected by the enclosure aspect ratio when A P 1 because then there will be always a single lattice in the vertical direction (no change in the geometry of the vertical direction); however, when A < 1 Eq. (17) indicates N minÀv to be proportional to A 2 , with the vertical interference becoming more likely as A decreases. This is so because when A decreases the number of lattices stacked in the vertical direction increases proportionally, which is equivalent in effect to an increase in the enclosure height.…”
Section: Minð1; Aþmentioning
confidence: 95%
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“…(17), N minÀv is not affected by the enclosure aspect ratio when A P 1 because then there will be always a single lattice in the vertical direction (no change in the geometry of the vertical direction); however, when A < 1 Eq. (17) indicates N minÀv to be proportional to A 2 , with the vertical interference becoming more likely as A decreases. This is so because when A decreases the number of lattices stacked in the vertical direction increases proportionally, which is equivalent in effect to an increase in the enclosure height.…”
Section: Minð1; Aþmentioning
confidence: 95%
“…The difference between Eqs. (17) and (19) is the extra A factor in the denominator of Eq. (19), leading to N minÀv /N minÀh = A.…”
Section: Minð1; Aþmentioning
confidence: 99%
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“…The case of a porous medium formed by a number of randomly distributed solid obstacles is studied by Pourshaghaghy et al (2007) whereas Hooman and Gurgenci (2010) studied flow through a finned-tube bundle modeled as a designed porous medium. Braga and de Lemos (2005a,b) analyzed regularly distributed particles by comparing the low-resolution volumeaveraged porous medium model with an enclosure bathing disconnected and conducting solid blocks.…”
mentioning
confidence: 99%