Handbook of Porous Media 2015
DOI: 10.1201/b18614-23
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Analyzing Nano“uids Suspension Using the Porous Media Interface Heat Transfer Model

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Cited by 6 publications
(7 citation statements)
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“…When Rb = 24 in Fig. 3, the streamlines within the nonstagnant region are mostly almost vertical or almost horizontal, apart from close to teh corners, and therefore the network model developed in Rees (2015a) is of some relevance. In that chapter, the square porous cavity was assumed to consist of narrow vertical and horizontal channels of equal width which were arranged in a square network.…”
Section: Figure 3 Near Herementioning
confidence: 97%
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“…When Rb = 24 in Fig. 3, the streamlines within the nonstagnant region are mostly almost vertical or almost horizontal, apart from close to teh corners, and therefore the network model developed in Rees (2015a) is of some relevance. In that chapter, the square porous cavity was assumed to consist of narrow vertical and horizontal channels of equal width which were arranged in a square network.…”
Section: Figure 3 Near Herementioning
confidence: 97%
“…where the value, G, is the threshold pressure gradient. If a porous medium were to be composed of a parallel set of identical channels of width, h, then Rees (2015a) shows that the threshold gradient is given by G = 2τ 0 /h where τ 0 is the yield stress of the fluid. An almost identical formula for G applies when the microstructure is composed of tubes of circular cross-section.…”
Section: The Darcy-bingham Lawmentioning
confidence: 99%
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“…Unlike Herschel-Bulkeley and Casson fluids, they exhibit a linear stress-strain relationship once the yield stress is exceeded. They arise in a wide variety of situations both in the environment and industry, and examples of the very many natural and man-made fluids which exhibit a yield stress have been collated and prsented in the chapter [1].…”
Section: Introductionmentioning
confidence: 99%