Elucidating the ${}^1$H NMR relaxation mechanism in polydisperse polymers and bitumen using measurements, MD simulations, and models

Abstract

The mechanism behind the ${}^1$H NMR frequency dependence of $T_1$ and the viscosity dependence of $T_2$ for polydisperse polymers and bitumen remains elusive. We elucidate the matter through NMR relaxation measurements of polydisperse polymers over an extended range of frequencies ($f_0=0.01\leftrightarrow$ 400 MHz) and viscosities ($\eta =385\leftrightarrow 102,000$ cP) using $T_1$ and $T_2$ in static fields, $T_1$ field-cycling relaxometry, and $T_{1\rho }$ in the rotating frame. We account for the anomalous behavior of the log-mean relaxation times $T_{1LM}\propto f_0$ and $T_{2LM}\propto (\eta /T{)}^{-1/2}$ with a phenomenological model of ${}^1$H-${}^1$H dipole-dipole relaxation which includes a distribution in molecular correlation times and internal motions of the non-rigid polymer branches. We show that the model also accounts for the anomalous $T_{1LM}$ and $T_{2LM}$ in previously reported bitumen measurements. We find that molecular dynamics (MD) simulations of the $T_1\propto f_0$ dispersion and $T_2$ of similar polymers simulated over a range of viscosities ($\eta =1\leftrightarrow 1,000$ cP) are in good agreement with measurements and the model. The $T_1\propto f_0$ dispersion at high viscosities agrees with previously reported MD simulations of heptane confined in a polymer matrix, which suggests a common NMR relaxation mechanism between viscous polydisperse fluids and fluids under confinement, without the need to invoke paramagnetism.

References in corpus (1)

• Molecular Dynamics Simulations of NMR Relaxation and Diffusion of Bulk Hydrocarbons and Water