This is the authors' abstract. We don't add key points for this paper.
The structure of poly (ε-caprolactam) (nylon 6) in the β mesomorphic form is here examined. The comparison of the diffraction intensity, calculated on modeled structures, with the experimental profiles, collected by us through an automatic diffractometer, is presented. This analysis has put into evidence the following limiting structural features. (a) The β form of nylon 6 is made of small mesomorphic aggregates of chains (where the matter scatters coherently) with axes arranged in a hexagonal lattice ( a = b = 0.48 nm; γ = 120°). (b) The chains have disordered conformations (and do not have a definite chirality, as it is the case for the 2 1 helices in the α and γ forms) with the −CH 2 − chains close to nearly all- trans (antiperiplanar) and the two dihedral angles adjacent to the amide bond, ±120°) to antiperiplanar (180°). This notwithstanding, the chains are straight and extended. As a result, the mean chain periodicity is close to 0.835 nm. (c) The H-bonds are formed along lines in the [100], [010], and [11̄0] directions; they force neighboring chains within the small mesomorphic aggregates to adjust their conformation in such a way that nearly 100% of hydrogen bonds are always formed, in agreement with the IR data. In the case of the α and γ more ordered forms of nylon 6, such lines are all in a unique direction, leading to hydrogen-bonded sheets (parallel to the chain axis) of enantiomorphous anticlined, alternately up and down chains (in the α form) or of isomorphous isoclined chains, (in the γ form). (d) As a consequence, since the amide groups lie all at nearly the same height along z, in the β form of nylon 6 the lines of hydrogen bonds lie in layers perpendicular to the chain axis and have the same direction within each layer. However, consecutive layers along z may have the lines of H-bonds which are not parallel (e.g., occasionally rotated by +120 or −120° instead of the “normal” 180°). (e) In the β form of nylon 6, disorder arises also from the random substitution of up and down chains in the lattice positions.
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Auriemma et al. (1997) studied this question.
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