2023
DOI: 10.1016/j.commatsci.2022.111824
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Linear viscoelastic shear and bulk relaxation moduli in poly(tetramethylene oxide) (PTMO) using united-atom molecular dynamics

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Cited by 5 publications
(4 citation statements)
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“…The UA potential used in the reference system is the Transferable Potentials for Phase Equilibria-UA (TraPPE-UA) for the intra (bonded) and inter-molecular (nonbonded) interactions initially developed by Lempesis et al 3 . Shireen et al further validated and established the TraPPE-UA potentials to study shear and bulk relaxation behavior of melt PTMO 70 . Before collecting data, the system was equilibrated at T = 453 K for 5 ns in a canonical ensemble using the deterministic Nose-Hoover thermostat 71,72 .…”
Section: Simulation Detailsmentioning
confidence: 99%
“…The UA potential used in the reference system is the Transferable Potentials for Phase Equilibria-UA (TraPPE-UA) for the intra (bonded) and inter-molecular (nonbonded) interactions initially developed by Lempesis et al 3 . Shireen et al further validated and established the TraPPE-UA potentials to study shear and bulk relaxation behavior of melt PTMO 70 . Before collecting data, the system was equilibrated at T = 453 K for 5 ns in a canonical ensemble using the deterministic Nose-Hoover thermostat 71,72 .…”
Section: Simulation Detailsmentioning
confidence: 99%
“…Conventionally, reaction limited cluster aggregation (RLCA) is distinguished from DLCA with m ∝ R g d f = 2.0 and N ( m ) ∝ m –τ=1.0 . To differentiate the structures observed in RLCA systems and lattice animals in this study, we further analyze the chemical distance (similar to the end-to-end distance in polymer models 38 ) in A clusters at all flexibility values. The chemical distance l is the length of the shortest path between two monomers of a cluster.…”
Section: Resultsmentioning
confidence: 99%
“…We note that these systems are strongly dynamically arrested due to the lack of rearrangements in local and mesoscale order rather than chain-scale dynamics. Particle-based simulations often cannot reach the required time scales to fully access the relaxation dynamics of entangled linear polymer melts, but simulations of typical entangled melts show a slow decay on G ( t ). However, in these SCLCP systems at low T , the G ( t ) curves are relatively flat without a transitional regime (the modulus change with time is subtle) compared to entangled linear polymer melts due to the morphology constraints imposed by LC moieties. , …”
Section: Resultsmentioning
confidence: 99%
“…At lower temperatures (T < 2.0 ε/k B ), there is no transitional behavior observed at intermediate time scales, unlike in entangled linear polymer melts. 61,63 Instead, the relaxation modulus spectra display a flat profile with a power law close to 0, extending to longer time scales. This highly non-Newtonian behavior is attributed to the slow dynamics resulting from the formation of crystalline networks or, in the case of systems with random LC sequences, to chains' arrested motion due to highly disrupted structures (Figure 4).…”
mentioning
confidence: 96%