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Hindered Rotation in Ethyl Alcohol

dc.contributor.authorHalford, J. O.en_US
dc.date.accessioned2010-05-06T21:45:21Z
dc.date.available2010-05-06T21:45:21Z
dc.date.issued1949-02en_US
dc.identifier.citationHalford, J. O. (1949). "Hindered Rotation in Ethyl Alcohol." The Journal of Chemical Physics 17(2): 111-117. <http://hdl.handle.net/2027.42/70179>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70179
dc.description.abstractPrevious evaluations of the barriers hindering the internal rotations in ethyl alcohol are shown to be unsatisfactory because they fail to produce agreement between molecular and calorimetric entropies over a wide enough temperature range. The principal source of difficulty is found in an inconsistency between the modified Berthelot equation of state and the calorimetric data and vapor pressures used in calculating the third law entropies. Corrections for gas imperfection should be much higher at the temperatures at which the barrier evaluations have been made, but these corrections cannot be determined accurately with the available data. The larger entropies permit the assignment of lower and more reasonable potential barriers.For the hydroxyl group rotation, to keep the heat capacity, and therefore the change of entropy with the temperature, within the indicated limits, the simple expression V = V0(1—cos3θ)/2 is more suitable than more detailed potential energy functions. With a reasonable assignment of the vibrational frequencies, the sum of the barriers restricting the hydroxyl and methyl group rotations is approximately 6000 cal.en_US
dc.format.extent3102 bytes
dc.format.extent490444 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.titleHindered Rotation in Ethyl Alcoholen_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/2027.42/70179/2/JCPSA6-17-2-111-1.pdf
dc.identifier.doi10.1063/1.1747203en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceJ. O. Halford, J. Chem. Phys. 15, 645 (1947); 16, 410 (1948); 16, 560 (1948).en_US
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dc.identifier.citedreferenceS. C. Schumann and J. G. Aston, J. Chem. Phys. 6, 480 (1938).en_US
dc.identifier.citedreferenceJ. G. Aston, Ind. Eng. Chem. 34, 514 (1942).en_US
dc.identifier.citedreferenceK. K. Kelley, J. Am. Chem. Soc. 51, 779 (1929).en_US
dc.identifier.citedreferenceE. F. Fiock, D. C. Ginnings, and W. B. Holton, J. Research Nat. Bur. Stand. 6, 881 (1931).en_US
dc.identifier.citedreferenceK. S. Pitzer and W. D. Gwinn, J. Chem. Phys. 10, 428 (1942).en_US
dc.identifier.citedreferenceJ. O. Halford, L. C. Anderson, and G. H. Kissin, J. Chem. Phys. 5, 927 (1937).en_US
dc.owningcollnamePhysics, Department of


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