Bj. Lommerts et al., STRUCTURE AND MELTING OF PERFECTLY ALTERNATING ETHYLENE CARBON-MONOXIDE COPOLYMERS, Journal of polymer science. Part B, Polymer physics, 31(10), 1993, pp. 1319-1330
The perfectly alternating ethylene carbon monoxide copolymer (polyketo
ne; POK) has been studied by means of H-1 nuclear magnetic resonance a
nd thermal analysis, and the crystal structure, determined by wide ang
le x-ray scattering methods, is presented. The crystal structure of th
is polymer in well-oriented fibers (POK-alpha) is as follows: Space gr
oup Pbnm, a = 6.91 (2) angstrom, b = 5.12 (2) angstrom, c = 7.60 (3) a
ngstrom (fiber axis), rho(c) = 1383 kg/m3. This differs from the struc
ture reported earlier by Chatani et al. (POK-beta). The very dense pac
king in the POK-alpha structure is a result of the arrangement of the
dipoles in the crystal lattice, giving rise to strong lateral forces b
etween the polymer chains. Owing to the all-trans conformation of the
polymer chain in the crystal lattice, high moduli can be achieved for
well-oriented fibers. A first approximation results in a value of 360
GPa for the theoretical modulus. From the melting data for a series of
low molecular weight polyketone homologs, a first, estimate is derive
d for the crystalline heat of fusion (215-330 J/g) for infinite chain
length. As a result of the strong lateral forces, this polymer shows a
(very) high crystalline heat of fusion, whereas creep and compressive
strength of oriented fibers are expected to be superior to those of h
igh-modulus polyethylene fibers. (C) 1993 John Wiley & Sons, Inc.