1988
DOI: 10.1016/0009-2509(88)80056-3
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Modelling of heat transfer at the wall of a packed-bed apparatus

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Cited by 31 publications
(22 citation statements)
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“…Yagi and Kunii (1961) elaborated on their earlier ideas of a discontinuous boundary layer to obtain: where α = 2.6 for liquids and 4.0 for gases. Note that a later development (Tobis and Ziolkowski, 1988) generalised this theory and unified the results for both gases and liquids. For Nu w0 Yagi and Kunii (1961) adapted their earlier stagnant conductivity model (Yagi and Kunii, 1957) assuming a near‐wall thickness of d p /2 and taking near‐wall voidage ε w = 0.7.…”
Section: Wall Heat Transfer Coefficientmentioning
confidence: 65%
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“…Yagi and Kunii (1961) elaborated on their earlier ideas of a discontinuous boundary layer to obtain: where α = 2.6 for liquids and 4.0 for gases. Note that a later development (Tobis and Ziolkowski, 1988) generalised this theory and unified the results for both gases and liquids. For Nu w0 Yagi and Kunii (1961) adapted their earlier stagnant conductivity model (Yagi and Kunii, 1957) assuming a near‐wall thickness of d p /2 and taking near‐wall voidage ε w = 0.7.…”
Section: Wall Heat Transfer Coefficientmentioning
confidence: 65%
“…Despite the existence of the more general mechanistic formula, further studies have reinforced the idea that h w = h w0 + a Re b or sometimes simply h w = a Re b alone (Specchia et al, 1980; Ziolkowski and Legawiec, 1987; Peters et al, 1988; Borkink and Westerterp, 1992; Martin and Nilles, 1993; Bey and Eigenberger, 2001). The formula of Yagi and Kunii (1960) was re‐visited by Tobis and Ziolkowski (1988), but their main interest was in ${\rm Nu}_{{\rm w}}^{*} $ , as they began a line of research in which only the film coefficient $h_{{\rm w}}^{*} $ was retained in the wall boundary condition. Nevertheless, they showed that using Equation (19) with a reasonable range of values of Nu w0 could account for much of the spread in Nu w , as shown in Figure 9.…”
Section: Wall Heat Transfer Coefficientmentioning
confidence: 99%
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“…The observed variation in porosity discussed in section 2.12, along with a prescription of D.J..(x), has been used by Cheng and Rsu (1986a,b), Cheng and Zhu (1987), and . A similar approach is used by Tobis and Ziolkowski (1988).…”
Section: Models Based On Mixing-length Theorymentioning
confidence: 99%
“…The flow state is divided into: Darcy flow: Re <1; Inertial flow: 1<Re<150; Unstable laminar flow: 150 <Re <300; and Turbulent flow: Re> 300 (Jolls & Hanratty 1966;Tobiś & Ziółkowski 1988). For the heat transfer characteristics, Wakao and Funazkri (1978) summarized the convective heat transfer criterion formula inside the packed bed: Nu = 2 + 1.1Pr…”
Section: Halaju Bekalan Udara Adalah Faktor Penting Yang Mempengaruhimentioning
confidence: 99%