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Dipole Moments of Dimethylsiloxane Oligomers and Poly(dimethylsiloxane)

dc.contributor.authorSutton, C.en_US
dc.contributor.authorMark, J. E.en_US
dc.date.accessioned2010-05-06T20:37:51Z
dc.date.available2010-05-06T20:37:51Z
dc.date.issued1971-06-15en_US
dc.identifier.citationSutton, C.; Mark, J. E. (1971). "Dipole Moments of Dimethylsiloxane Oligomers and Poly(dimethylsiloxane)." The Journal of Chemical Physics 54(12): 5011-5014. <http://hdl.handle.net/2027.42/69456>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/69456
dc.description.abstractDielectric constants at 20, 30, 40, and 50°C have been determined for pure liquid dimethylsiloxane oligomers (CH3)3Si–[OSi(CH3)2]xOSi(CH3)3 having chain lengths corresponding to x  =  3,5,7,and9x=3,5,7,and9. Mean‐square dipole moments ⟨μ2⟩⟨μ2⟩, calculated from the Onsager equation, are in good agreement with predicted values based on a rotational isomeric state model with neighbor dependence and chain conformational energies obtained in an independent analysis of the random‐coil dimensions of such chains. In addition, the observed temperature coefficients of ⟨μ2⟩⟨μ2⟩ are in qualitative agreement with calculated results for the stated range of xx. An experimental value of the ratio ⟨μ2⟩ / nm2⟨μ2⟩∕nm2 (where nn is the number of bond dipoles, each of magnitude mm) in the limit of large xx is estimated from published data on the pure liquid polymer at 25°C. This tentative result is in fair agreement with theory; agreement is improved if the large specific solvent effect previously observed for this polymer is interpreted as being primarily due to the effect of the dielectric constant of the medium on the Coulombic contribution to the conformational energy.en_US
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleDipole Moments of Dimethylsiloxane Oligomers and Poly(dimethylsiloxane)en_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, Michigan 48104en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/69456/2/JCPSA6-54-12-5011-1.pdf
dc.identifier.doi10.1063/1.1674790en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
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dc.identifier.citedreferenceP. J. Flory, Statistical Mechanics of Chain Molecules (Interscience, New York, 1969).en_US
dc.identifier.citedreferenceThese samples were generously provided by Dr. T. Williams of the Union Carbide Corp. and Dr. J. Saam of the Dow‐Corning Corp.en_US
dc.identifier.citedreferenceConstructed by the Wissenschaftlich‐Technische Werkstätten, GMBH, Weilheim Oberbayern, Germany; available in the United States from the Kahl Scientific Instrument Co., El Cajon, Calif.en_US
dc.identifier.citedreferenceC. P. Smyth, Dielectric Behavior and Structure (McGraw‐Hill, New York, 1955), p. 405.en_US
dc.identifier.citedreferenceL. Onsager, J. Am. Chem. Soc. 58, 1486 (1936).en_US
dc.identifier.citedreferenceThere are two errors in the description of this calculation in Ref. 11: a unit matrix of order three should replace the last statistical‐weight matrix UaUa appearing in Eq. (6) and should also replace the UaUa appearing in the last generator matrix GaGa in Eq. (8).en_US
dc.identifier.citedreferenceAmerican Institute of Physics Handbook, edited by D. E. Gray et al. (McGraw‐Hill, New York, 1963).en_US
dc.owningcollnamePhysics, Department of


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