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Growth of a Diffusion Flame in the Field of a Vortex

Marble, F. E. (1985) Growth of a Diffusion Flame in the Field of a Vortex. In: Recent advances in the aerospace sciences. Plenum Press , New York, pp. 395-413. ISBN 0306410796 http://resolver.caltech.edu/CaltechAUTHORS:20101207-085326836

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Abstract

A simple diffusion flame with fast chemical kinetics is initiated along the horizontal axis between a fuel occupying the upper half-plane and an oxidizer below. Simultaneously a vortex of circulation T is established at the origin. As time progresses the flame is extended and "wound up" by the vortex flow field and the viscous core of the vortex spreads, converting the motion in the core to a solid-body rotation. The kinematics of the flame extension and distortion is described and the effect of the local-flow field upon local-flame structure is analyzed in detail. It is shown that the combustion field consists of a totally reacted core region, whose radius is time dependent, and an external flame region consisting of a pair of spiral arms extending off at large radii toward their original positions on the horizontal axis. The growth of the reacted core, and the reactant-consumption rate augmentation by the vortex field in both core and outer-flame regions were determined for values of the Reynolds number (T/2πv) between 1 and 10^3 and for a wide range of Schmidt numbers (v / D) covering both gas and liquid reactions. For large values of Reynolds number the radius r _* of the reactant grows much more rapidly than the viscous core so that only the nearly inviscid portion of the flow is involved. The more accurate condition for this behavior is that R(Sc)^(1/2)>50 and, under this restriction, the similarity rule for the core radius growth is shown to be r _*(T^(2/3)D^(1/3)t)^(1/2)=0.5092+O(D/T)^(1/2) In this case also the reactant consumption rate becomes independent of time and, for the complete diffusion flame in the vortex field, the augmentation of reactant-consumption rate due to the vortex field satisfies Augmented consumption rate == 1. 2327 ,-1.4527(D/T)^(1/6) + O(D/T)^(1/2) T^(2/3) D^(1/3) Both of these similarity rules are, as is appropriate for high Reynolds number, independent of kinematic viscosity.


Item Type:Book Section
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http://md1.csa.com/partners/viewrecord.php?requester=gs&collection=TRD&recid=A8547320AH&q=related%3ARnfD4cztis8J%3Ascholar.google.com%2F&uid=790135166&setcookie=yesOtherUNSPECIFIED
Additional Information:© 1985, New York, Plenum Press. This work was supported, in part, by grant AFOSR-80-0265 and by NASA grant NAG 3-70.
Group:Guggenheim Jet Propulsion Center
Funders:
Funding AgencyGrant Number
Air Force Office of Scientific Research (AFOSR)AFOSR-80-0265
NASANAG 3-70
Subject Keywords:COMBUSTIBLE FLOW | DIFFUSION FLAMES | FLAME PROPAGATION | FUEL COMBUSTION | VORTICES | FUEL CONSUMPTION | REACTION KINETICS | REYNOLDS NUMBER | SCHMIDT NUMBER
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Other Numbering System NameOther Numbering System ID
Guggenheim Jet Propulsion CenterUNSPECIFIED
CSA IlluminaA85-47304 23-31
Record Number:CaltechAUTHORS:20101207-085326836
Persistent URL:http://resolver.caltech.edu/CaltechAUTHORS:20101207-085326836
Official Citation:Growth of a diffusion flame in the field of a vortex / MARBLE, F E. Recent advances in the aerospace sciences (A85-47304 23-31). New York, Plenum Press, 1985, p. 395-413
Usage Policy:No commercial reproduction, distribution, display or performance rights in this work are provided.
ID Code:21207
Collection:CaltechAUTHORS
Deposited By: Ruth Sustaita
Deposited On:14 Dec 2010 22:25
Last Modified:26 Dec 2012 12:43

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