1981
DOI: 10.1016/0017-9310(81)90157-5
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Heat conduction in spheres packed in an infinite regular cubical array

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Cited by 50 publications
(23 citation statements)
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“…The standard deviation for the expected b value can be attributed to the fact that the particles may have a shape other than spherical (in fact, they are hexagonal nanocrystallites, wurzite phase) 14 as stated by Parott and Stuckes. 20 According to these and other authors, [21][22][23][24] for porous solid materials b can be considered as a structural value for which various values can be found experimentally. The same should be true for other kind of composite materials such as nanofluids.…”
Section: Resultsmentioning
confidence: 99%
“…The standard deviation for the expected b value can be attributed to the fact that the particles may have a shape other than spherical (in fact, they are hexagonal nanocrystallites, wurzite phase) 14 as stated by Parott and Stuckes. 20 According to these and other authors, [21][22][23][24] for porous solid materials b can be considered as a structural value for which various values can be found experimentally. The same should be true for other kind of composite materials such as nanofluids.…”
Section: Resultsmentioning
confidence: 99%
“…The challenges in modeling complex materials come mainly from the inherent variety and randomness of their internal microstructures, and the coupling between the components of different phases. In literature, several attempts have been made to develop expressions for effective thermal conductivity of two-phase materials by various researchers such as, Maxwell [1], Lewis and Nielsen [2], Cunningham and Peddicord [3], Torquato [4], Hadley [5], Agari and Uno [6], Misra et al [7], Singh and Kasana [8], and Verma et al [9]. Lewis and Nielsen [2] reported a semi-empirical model incorporating the effect of the shape and the orientation of particles or, the type of packing for a two-phase system.…”
Section: Introductionmentioning
confidence: 99%
“…A plot of the blister threshold data for representative plate type fuels is shown in Figure 21. 22 At the end of irradiation the AFIP-6 fuel plates were estimated to reach fission densities greater than 3u10 21 f/cc with peaks as high as ~3.5u10 21 f/cc. At this fission density blistering could be anticipated to occur in regions of the fuel plate operating at temperatures as low as ~400ºC.…”
Section: Experiments Designmentioning
confidence: 99%
“…The thermal conductivity can then be corrected to account for porosity 21 using K P K 100 e 2.14 P where k P is the thermal conductivity of the porous materials, k 100 is the thermal conductivity of the fully-dense material, and P is porosity.…”
Section: Experiments Designmentioning
confidence: 99%