1965
DOI: 10.1007/bf00828695
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Laws of ignition of condensed explosive systems with perfect heat transfer at the surface and allowance for burnup

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Cited by 15 publications
(5 citation statements)
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“…Guidance concerning the accuracy to be expected from the asymptotic expansion may be sought by comparing the asymptotic results with those obtained from numerical Table 1 for the zero-flux time at 0, = 10 and at 0, = 25, where (39) and (40) are claimed to be good, reveal differences between the correlation and the numerical integration of [6] that are on the order of 15%, considerably greater than the stated error of the correlations [5]. Results of the four term expansion for f a with a = 0 lie between those of the two numerical studies but quite close to the results of [6].…”
Section: Results and Comparisons The Results Having Greatest Interesmentioning
confidence: 99%
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“…Guidance concerning the accuracy to be expected from the asymptotic expansion may be sought by comparing the asymptotic results with those obtained from numerical Table 1 for the zero-flux time at 0, = 10 and at 0, = 25, where (39) and (40) are claimed to be good, reveal differences between the correlation and the numerical integration of [6] that are on the order of 15%, considerably greater than the stated error of the correlations [5]. Results of the four term expansion for f a with a = 0 lie between those of the two numerical studies but quite close to the results of [6].…”
Section: Results and Comparisons The Results Having Greatest Interesmentioning
confidence: 99%
“…To account for effects of reactant consumption with a first-order reaction, (3) and (4) s /(Eq), a measure of the magnitude of the effect of reactant consumption, and the Lewis number L, the ratio of heat to reactant diffusivities. This problem was studied previously for nondiffusive reactants (L = oo) by numerical integration of the partial differential equations [5]. For L = oo, the last boundary condition in (A2) is deleted; for finite L this condition represents vanishing of the diffusive flux of reactant at the surface.…”
Section: Discussionmentioning
confidence: 99%
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“…In the cited studies, the burnout of the RM was not taken into account [4,[6][7][8] or was considered in a limited range of system parameters [2,3,5]. At the same time, during high-temperature ignition, as shown by Averson et al [9] for the problem of ignition by a hot wall, the burnout of the RM near the hot surface can result in a change in the initiation conditions, leading to the need for an additional determination of the ignition conditions. In the case of high-temperature ignition by a hot inert body with a finite heat reserve, the burnout of the RM can have a significant effect on both the initiation regimes and the critical parameters of the system.…”
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confidence: 99%
“…This condition corresponded to a qualitative change in the behavior of the temperature of the hot surface: after the initial decrease due to heat transfer to the RM, the surface temperature of the inert body begins to increase due to the heat of chemical reactions in the RM. However, as shown in [3,9], for hightemperature ignition regimes, the last fourth criterion is unacceptable since, near the hot surface of the particle, the reactive material burns out immediately upon contact. Because the present study deals with regimes involving the burnout of the reactant, the last criterion, according to the conclusion in [3], was not used further.…”
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confidence: 99%