1960
DOI: 10.1016/s0010-2180(60)80042-9
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Ignition of cellulosic materials by radiation

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Cited by 73 publications
(34 citation statements)
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“…It is certain, from this graphical presentation, that an increase of air flow in the range of (1.5-4.5) l min À1 leads to considerably longer ignition delay times, due to the increased sample cooling, as well as to the decreased concentration of fuel vapors in the boundary layer. The above findings are consistent with those reported by other authors [18,19]. Fig.…”
Section: The Effect Of Air Flow Around the Specimensupporting
confidence: 94%
See 1 more Smart Citation
“…It is certain, from this graphical presentation, that an increase of air flow in the range of (1.5-4.5) l min À1 leads to considerably longer ignition delay times, due to the increased sample cooling, as well as to the decreased concentration of fuel vapors in the boundary layer. The above findings are consistent with those reported by other authors [18,19]. Fig.…”
Section: The Effect Of Air Flow Around the Specimensupporting
confidence: 94%
“…In contrast, other researchers obtained longer ignition times for smaller samples. They attributed this to the fact that for small samples the fuel vapors, emerging through the surface of solid fuel, are of relatively low concentration, insufficient to promote ignition [18]. By plotting fire point values versus sample size (Fig.…”
Section: The Influence Of Sample Sizementioning
confidence: 99%
“…This was evidently a gas-phase effect, but even today there is no systematic knowledge on gas-phase ignition effects. In another study [68], Simms concluded that the quantitative effect of the rather small exposure size of 8 mm is nearly negligible, so presumably the enormous min q & ′ ′ values in the 1961 study were mainly due to insufficiently long test time. Moran [15] examined the ignition of vertical panels of 6.4 mm thick ponderosa pine using an electric radiant panel and found min q & ′ ′ = 25 kW m -2 .…”
Section: Experimental Results On Autoignitionmentioning
confidence: 96%
“…It is found in Fig. 11 that the top surface temperatures increase at different rate as the thermal conductivities of species vary [39,40]. For example, the top surface temperature is 290°C for oak, 330°C for aspens and birch, and 390°C for pine at the time of 300 s. The degree of thermal decomposition of the samples is very different as a result of variation of heat conduction inside the samples, which is shown by the mass loss curves for the solid phase in Fig.…”
Section: Furnace Experimentsmentioning
confidence: 98%