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Characteristics of UC, ZrC, and (ZrC) (UC) as Thermionic Emitters

dc.contributor.authorPidd, R. W. (Robert Wallace)en_US
dc.contributor.authorGrover, G. M.en_US
dc.contributor.authorRoehling, D. J.en_US
dc.contributor.authorSalmi, E. W.en_US
dc.contributor.authorFarr, J. D.en_US
dc.contributor.authorKrikorian, N. H.en_US
dc.contributor.authorWitteman, W. G.en_US
dc.date.accessioned2010-05-06T22:45:56Z
dc.date.available2010-05-06T22:45:56Z
dc.date.issued1959-10en_US
dc.identifier.citationPidd, R. W.; Grover, G. M.; Roehling, D. J.; Salmi, E. W.; Farr, J. D.; Krikorian, N. H.; Witteman, W. G. (1959). "Characteristics of UC, ZrC, and (ZrC) (UC) as Thermionic Emitters." Journal of Applied Physics 30(10): 1575-1578. <http://hdl.handle.net/2027.42/70821>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70821
dc.description.abstractUranium carbide is found to have the property of high thermionic emission in the observed temperature range from 1400 to 1800°K. The parameters of the Richardson equation which can be used to fit the data are A=7.3×105 amp∕cm2 (°K)2 and ϕ=4.57 v. While these parameters accurately predict the observed saturated currents, it is doubtful that such anomalous values are of theoretical significance within the framework of the Richardson‐Dushman derivation. A solid solution form of uranium carbide and zirconium carbide gives substantially the same thermionic emission as uranium carbide, and for other reasons appears to be the more useful emitter. The carbides require no surface preparation or activation schedule for use as emitters.en_US
dc.format.extent3102 bytes
dc.format.extent324988 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.titleCharacteristics of UC, ZrC, and (ZrC) (UC) as Thermionic Emittersen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumRandall Laboratory of Physics, University of Michigan, Ann Arbor, Michiganen_US
dc.contributor.affiliationotherLos Alamos Scientific Laboratory, Los Alamos, New Mexicoen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70821/2/JAPIAU-30-10-1575-1.pdf
dc.identifier.doi10.1063/1.1735003en_US
dc.identifier.sourceJournal of Applied Physicsen_US
dc.identifier.citedreferenceGrover, Roehling, Salmi, and Pidd, J. Appl. Phys. 29, 1611 (1958).en_US
dc.identifier.citedreferenceD. L. Goldwater and R. E. Haddad, J. Appl. Phys. 22, 70 (1951).en_US
dc.owningcollnamePhysics, Department of


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