2019
DOI: 10.1016/j.colsurfb.2019.03.033
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Interfacial ordering of tristearin induced by glycerol monooleate and PGPR: A coarse-grained molecular dynamics study

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Cited by 10 publications
(5 citation statements)
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“…We performed coarse-grained simulations using the Martini v2.2 lipid force field. , This model has been used previously for PEO, DOTAP, and MO . Because the entire unit cell of the inverted bicontinuous phase contains too many molecules to be simulated in full, we focus on a small section of the inside of one of the water channels, which we cap by an elastically bound wall (harmonic bonds with r 0 = 0.2 nm, k = 500–2000 kJ mol –1 nm –2 depending on the number of PEO chains) made out of C1-type beads, which were scaled to σ = 0.32 nm and otherwise interact like conventional C1 beads, to prevent particles from crossing representing the lipid tails that would normally form the bilayer.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…We performed coarse-grained simulations using the Martini v2.2 lipid force field. , This model has been used previously for PEO, DOTAP, and MO . Because the entire unit cell of the inverted bicontinuous phase contains too many molecules to be simulated in full, we focus on a small section of the inside of one of the water channels, which we cap by an elastically bound wall (harmonic bonds with r 0 = 0.2 nm, k = 500–2000 kJ mol –1 nm –2 depending on the number of PEO chains) made out of C1-type beads, which were scaled to σ = 0.32 nm and otherwise interact like conventional C1 beads, to prevent particles from crossing representing the lipid tails that would normally form the bilayer.…”
Section: Methodsmentioning
confidence: 99%
“…46,47 This model has been used previously for PEO, 52 DOTAP, 53 and MO. 54 Because the entire unit cell of the inverted bicontinuous phase contains too many molecules to be simulated in full, we focus on a small section of the inside of one of the water channels, which we cap by an elastically bound wall (harmonic bonds with r 0 = 0.2 nm, k = 500−2000 kJ mol −1 nm −2 depending on the number of PEO chains) made out of C1-type beads, which were scaled to σ = 0.32 nm and otherwise interact like conventional C1 beads, to prevent particles from crossing representing the lipid tails that would normally form the bilayer. The wall elasticity was varied by tuning the harmonic potential spring constant from 500 to 2000 kJ/(mol × nm 2 ) to account for the elasticity decrease when adding PBD-PEO to a lipid membrane.…”
Section: ■ Conclusionmentioning
confidence: 99%
“…The decrease of interfacial dilatational viscoelasticity with the increase of strain amplitude was due to the damage of interfacial film caused by the large amplitude. The higher interfacial viscoelasticity of PGPR was attributed to the branched chains on the hydrophobic long chain, resulting in the formation of a disordered entangled chain-like layer between the PGPR molecules at the interface [33] and enhancing their inter-molecular interactions to increase the maximum value of dilatational viscoelastic modulus [34].…”
Section: Amplitude Sweepmentioning
confidence: 99%
“…chains on the hydrophobic long chain, resulting in the formation of a gled chain-like layer between the PGPR molecules at the interface [33] a inter-molecular interactions to increase the maximum value of dilat modulus [34]. -8The viscoelastic properties of interface film can be obtained by jous curve, which appears a straight line for the pure elastic interface that of the viscoelastic interface [26].…”
Section: Amplitude Sweepmentioning
confidence: 99%
“…The resulting structures were shown to act as nucleation templates for triglycerides. [ 21 ] Detailed molecular modeling studies on food‐relevant triglyceride systems were carried out by the Milano group. A coarse‐grained model for triglycerides was developed, [ 22 ] and a multiscale approach to studying the liquid‐solid transition of triglycerides was presented.…”
Section: Introductionmentioning
confidence: 99%