Flow Field of a Bunsen Flame
dc.contributor.author | Uberoi, Mahinder S. | en_US |
dc.contributor.author | Kuethe, Arnold M. | en_US |
dc.contributor.author | Menkes, H. R. | en_US |
dc.date.accessioned | 2010-05-06T22:40:56Z | |
dc.date.available | 2010-05-06T22:40:56Z | |
dc.date.issued | 1958-03 | en_US |
dc.identifier.citation | Uberoi, 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.uri | https://hdl.handle.net/2027.42/70768 | |
dc.description.abstract | The 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.extent | 3102 bytes | |
dc.format.extent | 1150542 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Flow Field of a Bunsen Flame | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | University of Michigan, Ann Arbor, Michigan | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70768/2/PFLDAS-1-2-150-1.pdf | |
dc.identifier.doi | 10.1063/1.1705875 | en_US |
dc.identifier.source | Physics of Fluids | en_US |
dc.identifier.citedreference | The 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.citedreference | M. S. Uberoi, J. Chem. Phys. 22, 1784 (1954). | en_US |
dc.identifier.citedreference | B. Lewis and G. von Elbe, J. Chem. Phys. 11, 75 (1943). | en_US |
dc.identifier.citedreference | R. M. Fristrom, J. Chem. Phys. 24, 888 (1956). | en_US |
dc.owningcollname | Physics, Department of |
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