In this work, we use computer simulations to demonstrate that there may be limits to which polymer polarity alone can be used to influence the ionic conductivity of salt-doped polymer electrolytes. Specifically, we use coarse-grained molecular dynamics simulations to probe the effect of the polarity of the polymer electrolyte upon ion mobilities and conductivities of dissolved salts. At low polymer polarities, increasing the polymer dielectric constant reduces ionic aggregation and the resultant correlated ionic motion, and increases the ionic conductivity. At higher polymer polarities, polymer−polymer and polymer−ion interactions slows polymer segmental dynamics, leading to a reduction in the conductivity of the electrolyte. As a consequence, ionic conductivity achieves an optimum at an intermediate polymer polarity.
We
use all-atom molecular dynamics simulations to study the effect
of polymer polarity, as quantified by the dielectric constant, on
the transport properties of lithium bis(trifluoromethylsulfonyl)imide
(LiTFSI) doped polyethers. Our results indicate that increasing the
host dielectric constant leads to a decrease in ionic cluster sizes
and reduction in correlated motion of oppositely charged ions. This
causes the ionic conductivity to more closely approach the Nernst-Einstein
limit in which ionic conductivity is only limited by the diffusivities
of Li+ and TFSI–. We compare our results
to recent experimental observations which demonstrate similar qualitative
trends in host polarity.
We report the results of atomistic molecular dynamics simulations on polymerized 1-butyl-3-vinylimidazolium-hexafluorophosphate ionic liquids, studying the influence of the polymer molecular weight on the ion mobilities and the mechanisms underlying ion transport, including ion-association dynamics, ion hopping, and ion-polymer coordinations. With an increase in polymer molecular weight, the diffusivity of the hexafluorophosphate (PF) counterion decreases and plateaus above seven repeat units. The diffusivity is seen to correlate well with the ion-association structural relaxation time for pure ionic liquids, but becomes more correlated with ion-association lifetimes for larger molecular weight polymers. By analyzing the diffusivity of ions based on coordination structure, we unearth a transport mechanism in which the PF moves by "climbing the ladder" while associated with four polymeric cations from two different polymers.
We probe the ion mobilities, transference numbers, and
inverse Haven ratio of ionic liquids and polymerized ionic liquids
as a function of their molecular weight using a combination of atomistic
equilibrium and nonequilibrium molecular dynamics simulations. In
contrast to expectations, we demonstrate that the inverse Haven ratio
increases with increasing degree of polymerization (N) and then decreases at larger N. For a fixed center
of mass reference frame, we demonstrate that such results arise as
a consequence of the strong cation–cation correlated motions,
which exceed (in magnitude) the self-diffusivity of cations. Together,
our findings challenge the premise underlying the pursuit of pure
polymeric ionic liquids as high transference number, single-ion conducting
electrolytes.
In spite of significant interest toward solid-state electrolytes owing to their superior safety in comparison to liquid-based electrolytes, sluggish ion diffusion and high interfacial resistance
A mono(μ-oxo)bis(alkylaluminum) (MOB) catalyst and initiator for epoxide polymerization, [(H 3 C) 2 NCH 2 CH 2 (μ 2 -O)Al(iBu) 2 •Al(iBu) 3 ] (1), produced a ca. 170-fold enhancement in epoxide polymerization rate over previously reported MOB initiators demonstrated with allyl glycidyl ether (AGE). This discovery reduces polymerization times to minutes. 1 exhibited an exponential dependence of polymerization rate on concentration, rather than an expected low integer order relationship. A proposed polymerization intermediate was identified via direct synthesis, isolation, kinetic comparison, and corroborating in situ spectroscopic evidence to be a symmetric bis((μ-alkoxo)dialkylaluminum) (BOD) with a characteristic R 3 N•AlR′ 3 (N−Al) adduct. The N−Al adduct on the BOD intermediate is proposed to act as a catalyst, whereas the aluminoxane ring is proposed to be the site of monomer enchainment on the basis of mass spectrometry and spectroscopic analysis of resultant polymer structure. The distinct catalytic and initiation/propagation functionalities were separated into separate species, and the catalytic activity of the N−Al adduct was demonstrated in the presence of a distinct aluminoxane initiator. Each 1 equiv of N−Al adduct relative to initiator resulted in an abrupt (ca. 5−10fold) increase in the polymerization rate of AGE. The resultant N−Al adduct catalyst represents a versatile tool for rapid functional macromolecular synthesis.
We study ternary polymer-polymer-salt blend electrolytes using coarsegrained molecular dynamics. We specifically examine the influence of the polymer hosts' incompatibility and polarity contrast on electrolyte ion transport characteristics. We find that, at moderate-to high-polarity contrasts, improving the miscibility of the polymer hosts by reducing their inherent incompatibility improves ionic transport, as measured by the ionic conductivity. However, contrary to expectations, ionic conduction slows with increased miscibility in low-polarity contrast electrolytes. Upon examining the underlying material properties, we find that ionic aggregation exhibits trends similar to ionic conductivity and is thus likely the controlling factor in these polymer-blend electrolytes. Our results suggest that ionic conduction can be improved in real polymer electrolytes by choosing chemistries that promote simultaneous miscibility and polarity contrast between the polymer hosts.
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