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image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao The University of Ma...arrow_drop_down
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
zbMATH Open
Article . 1991
Data sources: zbMATH Open
image/svg+xml Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao Closed Access logo, derived from PLoS Open Access logo. This version with transparent background. http://commons.wikimedia.org/wiki/File:Closed_Access_logo_transparent.svg Jakob Voss, based on art designer at PLoS, modified by Wikipedia users Nina and Beao
SIAM Journal on Applied Mathematics
Article . 1991 . Peer-reviewed
Data sources: Crossref
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Transition from Thermal Runaway to Propagating Flames

Transition from thermal runaway to propagating flames
Authors: Henderson, KL; Dold, JW;

Transition from Thermal Runaway to Propagating Flames

Abstract

Summary: In analysing thermal runaway in reactive-diffusive systems, it can be seen that diffusion and conduction become significantly reduced in importance towards the final stages. As a result, these diffusive effects play a negligible role in the early structure of the reaction waves that finally emerge from an ignition kernel. These flames simply travel too fast to be genuinely self-propagating and move by virtue of the fact that the induction process causes some points to ignite before other points. It is convenient, therefore, to refer to these waves of chemical activity as ``induction flames''. As they slow down, however, diffusion becomes important again until, after an appropriate transition, self-propagating reaction waves are able to emerge. A simple unit Lewis number model is used to represent the final stage of thermal runaway via a temperature sensitive one-step exothermic reaction. With this, the progress of the transition from reaction runaway to self-propagating flames is described using a large activation energy asymptotic analysis.

Country
United Kingdom
Related Organizations
Keywords

self-propagating flames, large activation energy asymptotic analysis, Reaction-diffusion equations, Applications of PDE in areas other than physics, Classical flows, reactions, etc. in chemistry, Chemically reacting flows, induction, 004, Singular perturbations in context of PDEs

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selected citations
These citations are derived from selected sources.
This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
BIP!Impulse provided by BIP!
6
Average
Average
Average
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