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Flow Field of a Bunsen Flame
dc.contributor.authorUberoi, Mahinder S.en_US
dc.contributor.authorKuethe, Arnold M.en_US
dc.contributor.authorMenkes, H. R.en_US
dc.date.accessioned2010-05-06T22:40:56Z
dc.date.available2010-05-06T22:40:56Z
dc.date.issued1958-03en_US
dc.identifier.citationUberoi, M. S.; Kuethe, A. M.; Menkes, H. R. (1958). "Flow Field of a Bunsen Flame." Physics of Fluids 1(2): 150-158. <http://hdl.handle.net/2027.42/70768>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70768
dc.description.abstractThe flow field of a two‐dimensional Bunsen flame is examined by approximating the zone of combustion by a surface of discontinuity across which the density drops and normal velocity increases. Even though the flow of unburned gases is potential, the flow of the burned gases is always rotational and is therefore not amenable to complete analysis. Interaction of flame shape and flow field is obtained analytically and experimentally. The entire flow field of unburned and burned gases is mapped by taking stroboscopic photographs of small particles suspended in the combustible gases. The measured flow field is considered in the light of the above analysis.en_US
dc.format.extent3102 bytes
dc.format.extent1150542 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleFlow Field of a Bunsen Flameen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumUniversity of Michigan, Ann Arbor, Michiganen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70768/2/PFLDAS-1-2-150-1.pdf
dc.identifier.doi10.1063/1.1705875en_US
dc.identifier.sourcePhysics of Fluidsen_US
dc.identifier.citedreferenceThe equations of motion show that in general the vorticity of a fluid will change and it is conserved only under special circumstances. One is apt to regard the generation of vorticity as new, rather than classical, result since our knowledge of fluid flows is almost entirely limited to the potential or reversible case where the vorticity is zero everywhere. The generation of vorticity for the case of constant flame speed has been discussed by H. S. Tsien, J. Appl. Mech. 18, 188 (1951), and by R. A. Gross and R. Esch, Jet Propulsion 24, 95 (1954).en_US
dc.identifier.citedreferenceM. S. Uberoi, J. Chem. Phys. 22, 1784 (1954).en_US
dc.identifier.citedreferenceB. Lewis and G. von Elbe, J. Chem. Phys. 11, 75 (1943).en_US
dc.identifier.citedreferenceR. M. Fristrom, J. Chem. Phys. 24, 888 (1956).en_US
dc.owningcollnamePhysics, Department of


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