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1.
J Chem Phys ; 150(12): 124104, 2019 Mar 28.
Artigo em Inglês | MEDLINE | ID: mdl-30927875

RESUMO

A chain-revised Groot-Warren equation of state (crGW-EOS) was developed and tested to describe systems of homo-oligomeric chains in the framework of dissipative particle dynamics (DPD). First, thermodynamic perturbation theory is applied to introduce correction terms that account for the reduction in pressure with an increasing number of bonds at constant bead number density. Then, this EOS is modified by introducing a set of switching functions that yields an accurate second virial coefficient in the low-density limit. The crGW-EOS offers several improvements over the revised Groot-Warren equation of state and Groot-Warren equation of state for chain molecules. We tested the crGW-EOS by using it to predict the pressure of oligomeric systems and the B2 virial coefficient of chain DPD particles for a range of bond lengths. Additionally, a method is developed for determining the strength of cross-interaction parameters between chains of different compositions and sizes and for thermal and athermal mixtures. We explored how different levels of coarse-graining affect the upper-critical solution temperature.

2.
Langmuir ; 34(28): 8245-8254, 2018 07 17.
Artigo em Inglês | MEDLINE | ID: mdl-29902016

RESUMO

Understanding solute uptake into soft microstructured materials, such as bilayers and worm-like and spherical micelles, is of interest in the pharmaceutical, agricultural, and personal care industries. To obtain molecular-level insight on the effects of solutes loading into a lamellar phase, we utilize the Shinoda-Devane-Klein (SDK) coarse-grained force field in conjunction with configurational-bias Monte Carlo simulations in the osmotic Gibbs ensemble. The lamellar phase is comprised of a bilayer formed by triethylene glycol mono- n-decyl ether (C10E3) surfactants surrounded by water with a 50:50 surfactant/water weight ratio. We study both the unary adsorption isotherm and the effects on bilayer structure and stability caused by n-nonane, 1-hexanol, and ethyl butyrate at several different reduced reservoir pressures. The nonpolar n-nonane molecules load near the center of the bilayer. In contrast, the polar 1-hexanol and ethyl butyrate molecules both load with their polar bead close to the surfactant head groups. Near the center of the bilayer, none of the solute molecules exhibits a significant orientational preference. Solute molecules adsorbed near the polar groups of the surfactant chains show a preference for orientations perpendicular to the interface, and this alignment with the long axis of the surfactant molecules is most pronounced for 1-hexanol. Loading of n-nonane leads to an increase of the bilayer thickness, but does not affect the surface area per surfactant. Loading of polar additives leads to both lateral and transverse swelling. The reduced Henry's law constants of adsorption (expressed as a molar ratio of additive to surfactant per reduced pressure) are 0.23, 1.4, and 14 for n-nonane, 1-hexanol, and ethyl butyrate, respectively, and it appears that the SDK force field significantly overestimates the ethyl butyrate-surfactant interactions.

3.
Nanoscale ; 11(14): 6635-6643, 2019 Apr 04.
Artigo em Inglês | MEDLINE | ID: mdl-30895975

RESUMO

The self-assembly of amphiphilic graft copolymers is generally reported for polymer melts or polymers deposited onto surfaces, while a small number of cases deal with binary mixtures with water. We report on the associative properties of poly(ethylene glycol)-graft-poly(vinyl acetate) (PEG-g-PVAc) comb-like copolymers in water, demonstrating the existence of a percolative behaviour when increasing the PEG-g-PVAc content. Rheology, light- and small-angle X-ray scattering experiments, together with dissipative particle dynamics simulations, reveal a progressive transition from spherical polymer single-chain nanoparticles (SCNPs) towards hierarchically complex structures as the weight fraction of the polymer in water increases. The ability of PEG-g-PVAc to attain different nano- and microstructures is of great importance in numerous applications such as in the fields of cosmetics, detergency and drug delivery.

4.
J Colloid Interface Sci ; 556: 74-82, 2019 Nov 15.
Artigo em Inglês | MEDLINE | ID: mdl-31430708

RESUMO

HYPOTHESIS: Liquid-liquid phase separation (LLPS) can provide micron-sized liquid compartments dispersed in an aqueous medium. This phenomenon is increasingly appreciated in natural systems, e.g., in the formation of intracellular membraneless organelles, as well as in synthetic counterparts, such as complex coacervates and vesicles. However, the stability of these synthetic phase-separated microstructures versus coalescence is generally challenged by the presence of salts and/or surfactants, which narrows the range of possible applications. We propose a new strategy to obtain micron-sized liquid domains via LLPS, by mixing an amphiphilic copolymer with surfactants and sodium citrate in water at room temperature. EXPERIMENTS: Combining Confocal Laser Scanning Microscopy (CLSM) and Differential Scanning Calorimetry (DSC) with Dissipative Particle Dynamics (DPD) simulations, we map the phase diagram to detect LLPS and address the presence and morphology of these microscopic domains. This mapping in turn provides a first mechanistic hypothesis for the formation of such confined polymer-rich microenvironments. FINDINGS: LLPS is driven by the phase behavior of the copolymer in water and by its associative interactions with surfactants, combined with the water-sequestering ability of salting-out electrolytes. The key factor for LLPS and formation of microdomains is the entropy-driven dehydration of the copolymer head groups, which can be quantified through the Free Water Content (FWC). Interestingly, the internal morphology of the LLPS microdomains is finely controlled by the ratio between nonionic and anionic surfactants. Beside its applicative potential, this approach represents a tool for designing synthetic mimics that improve our understanding of the occurrence of LLPS in cells.

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