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Compressible Supersonic Flow in Jets under the Kármán‐Tsien Pressure‐Volume Relation

dc.contributor.authorCoburn, N.en_US
dc.date.accessioned2010-05-06T21:33:04Z
dc.date.available2010-05-06T21:33:04Z
dc.date.issued1951-02en_US
dc.identifier.citationCoburn, N. (1951). "Compressible Supersonic Flow in Jets under the Kármán‐Tsien Pressure‐Volume Relation." Journal of Applied Physics 22(2): 124-130. <http://hdl.handle.net/2027.42/70047>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70047
dc.description.abstractThe two‐dimensional supersonic irrotational flow of a gas in a jet is studied by use of the Kármán‐Tsien pressure‐volume law. There are two limitations to such a study: (1) since the fluid flow is not continued from the subsonic range, arbitrary boundary conditions must be prescribed; (2) use of the Kármán‐Tsien pressure‐volume relation implies a restriction on the permissible range of pressure, density, and velocity. On the other hand, use of the Kármán‐Tsien law furnishes several advantages: (1) the velocity potential and stream function satisfy the wave equation in the hodograph plane and hence these functions can be easily determined; (2) the mappings between the physical and hodograph planes may be completely characterized and studied in detail. This gain in information should be valuable in the qualitative understanding of phenomena as well as in obtaining first approximations to quantitative solutions. In the case of jets, with free stream lines as boundaries, it is shown that two functions possessing certain desired properties completely determine the Kármán‐Tsien flow. Further, the phenomenon of the periodic recurrence of the free stream jet boundary is explained by a folding property of the map of the flow in the hodograph plane.en_US
dc.format.extent3102 bytes
dc.format.extent551231 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.titleCompressible Supersonic Flow in Jets under the Kármán‐Tsien Pressure‐Volume Relationen_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/2027.42/70047/2/JAPIAU-22-2-124-1.pdf
dc.identifier.doi10.1063/1.1699912en_US
dc.identifier.sourceJournal of Applied Physicsen_US
dc.identifier.citedreferenceF. Frankl, Bull. Acad. Sci. U.R.S.S., Ser. Math. (Izvestia Akad. Nauk S.S.S.R.), 9, 121–143 (1945).en_US
dc.identifier.citedreferenceN. Coburn, Quart. Appl. Math. 3, No. 2 (July, 1945).en_US
dc.identifier.citedreferenceS. A. Chaplygin, “On gas jets,” Sci. Ann. Imp. Univ. Moscow, Physico‐Math. Division, Pub. No. 21 (Moscow, 1904), translated from the Russian by M. Slud (Brown University Notes, Providence, Rhode Island, 1944).en_US
dc.identifier.citedreferenceJ. D. Tamarkin and W. Feller, Partial Differential Equations (Brown University Notes, Providence, Rhode Island, 1941), pp. 24–28.en_US
dc.identifier.citedreferenceS. Bergman, Trans. Am. Math. Soc. 57, No. 3, 299–331 (May, 1945).en_US
dc.owningcollnamePhysics, Department of


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