We apply field cycling NMR to study segmental reorientation dynamics in melts of linear 1,4-polybutadiene (PB) in the entanglement regime ( M ≥ M e ). Dispersion data of the spin−lattice relaxation time T 1 (ω) are transformed to the susceptibility representation χ′′(ω) = ω/ T 1 (ω), and using frequency temperature superposition master curves χ′′(ωτ s ) are constructed which reflect spectral contributions from glassy as well as polymer specific dynamics. The correlation time τ s is determined by glassy dynamics. Transforming χ′′(ωτ s ) into the time domain and studying the crossover from Rouse to entanglement regime, the full dipolar or segmental reorientational correlation function F 2 ( t/τ s ) is presented covering six decades in amplitude and 8 decades in time. Assuming F 2 ( t ) ≅ ⟨ u b ( t ) u b (0)⟩ 2 the bond vector correlation function ϕ b ( t ) = ⟨ u b ( t ) u b (0)⟩ is obtained. Reaching Z = M/M e ≤ 9, comparison with theoretical predictions by the tube-reptation model as well as renormalized Rouse theory reveals significant discrepancies whereas good agreement is found with simulations. The crossover to entanglement dynamics appears to be very protracted.
No takes yet. Share an insight, caveat, or question.
Herrmann et al. (2009) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: