Answers are grounded in this paper and cite their sources.
The principal values of the 13 C chemical shift tensors and the 1 H− 13 C separated-local-field patterns are reported for the all-trans structures with long and short T 1 as well as the more and less mobile amorphous segments in polyethylene. It is shown that the principal values of the chemical shift tensor, and the local 1 H field of the tensor, for the all-trans crystalline structures with long and short T 1 are essentially the same, supporting the previous suggestion by Schmidt-Rohr and Spiess that chain diffusion between the amorphous and the crystalline regions in PE is the primary reason for the multiexponential 13 C T 1 relaxation observed for the all-trans peak observed at 33 ppm. The less mobile amorphous component adopts preferably a trans conformation and undergoes a fast rotation dominantly about the molecular axis at a rate larger than the width of the CH 2 group dipolar coupling. The motion involved in the mobile amorphous structure approaches isotropic tumbling, but a modest amount of constrained reorientation remains. Consequently, the 13 C− 1 H dipolar coupling is averaged out, but the shift tensor is not totally averaged to its isotropic value.
No takes yet. Share an insight, caveat, or question.
Hu et al. (2000) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: