2018
DOI: 10.1002/polb.24745
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Advancing the computational methodology of rigid rod and semiflexible polymer systems: A new solution to the wormlike chain model with rod‐coil copolymer calculations

Abstract: Jasiuk examine the broadening of glass transition in polymer nanocomposites. The cover image shows a bright-field transmission electron microscopy (TEM) image of the Aromatic thermosetting copolyester-Graphene Nanoplatelet (ATSP-GNP) nanocomposite. The ATSP fragments (darker) can be seen clinging to the GNP flakes (brighter), clearly displaying the extent of the effective attachment mechanism at the nanoscale.

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Cited by 6 publications
(5 citation statements)
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“…Nevertheless, this challenge can likely be overcome with new improved numerical methods. 58 We leave this for a future study.…”
Section: Discussionmentioning
confidence: 99%
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“…Nevertheless, this challenge can likely be overcome with new improved numerical methods. 58 We leave this for a future study.…”
Section: Discussionmentioning
confidence: 99%
“…When confronted with this problem, Tang et al resorted to solving the statistical mechanics of the single wormlike chain in w ( z , u ) using Monte Carlo simulations. Nevertheless, this challenge can likely be overcome with new improved numerical methods . We leave this for a future study.…”
Section: Discussionmentioning
confidence: 99%
“…Instead of the perfect symmetrical phase diagram of the coil−coil diblocks, the disorder−lamella transition point in the phase diagram is moved from the coil volume fraction f = 0.5 to a range between f = 0.6 and f = 0.65, which is also consistent with previous studies about the effect of orientation interactions and the geometrical asymmetry on the phase behavior of the rod−coil system. 52,68,71,72 From χN − f phase diagram of rod−coil blocks in the case of low-orientation interaction, we can see that a double continuous network structure DG appears in spite of complicated structures caused by the geometrical asymmetry and the orientation interaction. In the part of f ≤ 0.6, with the increase of the rigid composition, the proportion of DG in the phase diagram is larger, which is in sharp contrast to the coil− coil system.…”
Section: ■ Results and Discussionmentioning
confidence: 93%
“…[2] Originally,these concepts were predominantly applied to common surfactants and lipids, [3] but their validity is by no means limited to such compounds,and polymeric assemblies, when in thermodynamic equilibrium, satisfy the same description. [6] When the latter form closed shells,they are called vesicles,or, for polymers,"polymersomes". [5] When the hydrophilic-to-hydrophobic block length ratio decreases the curvature energies become smaller and one first encounters spheres,then rods,and finally lamellae.…”
mentioning
confidence: 99%
“…[5] When the hydrophilic-to-hydrophobic block length ratio decreases the curvature energies become smaller and one first encounters spheres,then rods,and finally lamellae. [6] When the latter form closed shells,they are called vesicles,or, for polymers,"polymersomes". [7] Arather special case are assemblies formed by oppositely charged polymers.…”
mentioning
confidence: 99%