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Thermodynamic Properties of the Internal Rotation in Methyl Alcohol Vapor from 200 to 500°K

dc.contributor.authorHalford, J. O.en_US
dc.date.accessioned2010-05-06T21:19:12Z
dc.date.available2010-05-06T21:19:12Z
dc.date.issued1950-08en_US
dc.identifier.citationHalford, J. O. (1950). "Thermodynamic Properties of the Internal Rotation in Methyl Alcohol Vapor from 200 to 500°K." The Journal of Chemical Physics 18(8): 1051-1056. <http://hdl.handle.net/2027.42/69898>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/69898
dc.description.abstractAt ordinary and lower temperatures the thermodynamic properties of the methyl alcohol internal rotation are beyond the limits of available tabulations. For any internal rotator, of a given symmetry, with a fixed moment of inertia and potential barrier, two limiting values of each property can be calculated for any chosen temperature. Available tables are restricted to those cases for which the differences between the limiting values can be neglected. When, as with methyl alcohol, the differences are large, the representative values can be found by taking proper account of the symmetry and the dependence of the internal rotator energy levels upon the external rotations.For methyl alcohol, the correct intermediate thermodynamic properties are obtained by using for the partition function and its derivatives the numerical mean of the limiting values of these sums obtained for the general rotator. This simple rule, however, is not necessarily applicable to other compounds.Heat capacities and entropies, calculated from the spectroscopic potential barrier of 932 cal./mole and other molecular constants, are considered in relation to experimental data.en_US
dc.format.extent3102 bytes
dc.format.extent501681 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.titleThermodynamic Properties of the Internal Rotation in Methyl Alcohol Vapor from 200 to 500°Ken_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumChemistry Department, University of Michigan, Ann Arbor, Michiganen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/69898/2/JCPSA6-18-8-1051-1.pdf
dc.identifier.doi10.1063/1.1747856en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceJ. O. Halford, J. Chem. Phys. 18, 361 (1950).en_US
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dc.identifier.citedreferenceJ. S. Koehler and D. M. Dennison, Phys. Rev. 57, 1006 (1940).en_US
dc.identifier.citedreferenceJ. O. Halford, J. Chem. Phys. 18, 444 (1950).en_US
dc.identifier.citedreferenceA. Eucken and E. U. Franck, Zeits. f. Elektrochemie 52, 195 (1948).en_US
dc.identifier.citedreferenceJ. S. Rowlinson, Nature 162, 820 (1948).en_US
dc.identifier.citedreferenceT. DeVries and B. T. Collins, J. Am. Chem. Soc. 63, 1343 (1941).en_US
dc.identifier.citedreferenceA. Eucken and L. Meyer, Zeits. f. Physik. Chemie 5B, 452 (1929).en_US
dc.owningcollnamePhysics, Department of


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