Molecular Vibrations and Structures of High Polymers. I. General Method of Normal Coordinate Treatment by Internal Coordinates and Infrared Frequencies and Conformations of (—CH2—)n, (—CH2–O—)n, and (—CH2–O–CH2—)n
- 1 August 1961
- journal article
- research article
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 35 (2) , 693-713
- https://doi.org/10.1063/1.1731990
Abstract
The normal coordinate treatment of the (—A—)n chain was made in terms of internal symmetry coordinates and optically active frequencies of (—CH2—)n were calculated for various chain conformations. The calculated frequencies of polyethylene and cyclopentane agreed with the observed values. The low infrared frequency was found to be structure sensitive. The infrared band of polytetrafluoroethylene at approx 100 cm—1 may be primarily due to this mode. The low infrared frequencies of polyoxymethylene were compared with the corresponding frequencies of (—A—)n calculated for various conformations and were found to be in accord with Huggins' model but not with the planar zigzag structure. The normal coordinate treatment of (—A—B—)n was made taking into account the torsional potential as well as the stretching and bending potentials, and vibrational assignments of polyoxymethylene were made. For poly‐(ethylene glycol) a structure model was proposed. This model is made up of only the gauche configuration throughout the helical chain and contains seven chemical units and five turns of the helix per fiber period. The polarized infrared spectra of this polymer were measured in the region 800–400 cm—1 and the observed skeletal frequencies were compared with the corresponding frequencies of (—A—)n calculated for various conformations. The infrared spectra were found to be in accord with the model proposed here. The infrared spectra in the rocksalt region were also reasonably assigned. Finally a general method of treating any infinite helical chain belonging to dihedral group is presented in terms of real internal symmetry coordinates. The G or F matrix of an infinite order is factored into the set of matrices G(δ) or F(δ) associated with the phase difference δ. The method is explained for the cases of polyoxymethylene and poly‐(ethylene glycol).Keywords
This publication has 31 references indexed in Scilit:
- The Infrared Spectra of Polypeptides in Various Conformations: Amide I and II Bands1Journal of the American Chemical Society, 1961
- Normal Vibrations of the Polymer Molecules of Helical ConfigurationThe Journal of Chemical Physics, 1960
- CH2 Rocking Frequencies of Ethylene Glycol and Its Derivatives in Relation to the Configuration of Polyethylene GlycolJournal of the American Chemical Society, 1960
- On the Helical Configuration of a Polymer ChainThe Journal of Chemical Physics, 1955
- The infra-red spectra of some optically active and meso -synthetic polypeptidesProceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 1954
- The vibration spectra of helical molecules: infra-red and Raman selection rules, intensities and approximate frequenciesProceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 1953
- The Normal Vibrations of Polyatomic Molecules as Calculated by Urey-Bradley Field. II. Vibrations of Polythene, Ethane, and Their Deuterium CompoundsThe Journal of Chemical Physics, 1949
- Raman Frequencies of n-Paraffin MoleculesJournal of the American Chemical Society, 1949
- The Normal Vibrations of Polyatomic Molecules as Treated by Urey-Bradley FieldThe Journal of Chemical Physics, 1949
- The Thermodynamics and Molecular Structure of Cyclopentane1Journal of the American Chemical Society, 1947