2015
DOI: 10.1016/j.chemphyslip.2014.06.006
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Modeling the interplay between protein and lipid aggregation in supported membranes

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Cited by 8 publications
(6 citation statements)
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“…How does this dissipated energy affect the membrane? There is experimental evidence that FtsZ filaments attached to a supported lipid bilayer affect the shape of lipid domains and that the segregated lipids also influence the distribution and shape of the filaments ( González de Prado Salas et al, 2015 ). Modeling this behavior requires considering filament torsion, monomer exchange, lateral interactions, and preferential curvature ( Gonzalez de Prado Salas et al, 2014 ), and the tendency of the lipids to segregate into domains ( Figure 2 ).…”
Section: Ftszmentioning
confidence: 99%
“…How does this dissipated energy affect the membrane? There is experimental evidence that FtsZ filaments attached to a supported lipid bilayer affect the shape of lipid domains and that the segregated lipids also influence the distribution and shape of the filaments ( González de Prado Salas et al, 2015 ). Modeling this behavior requires considering filament torsion, monomer exchange, lateral interactions, and preferential curvature ( Gonzalez de Prado Salas et al, 2014 ), and the tendency of the lipids to segregate into domains ( Figure 2 ).…”
Section: Ftszmentioning
confidence: 99%
“…41,42 Many other examples can be found. 28,[43][44][45][46] For these reasons, enzymatic conversion of proteins complicated by their aggregation is expected to be studied experimentally in the nearest future. From this perspective, the work presented herein can be classified as forefront research.…”
Section: Resultsmentioning
confidence: 99%
“…The particular choice of the arguments of the intermolecular potential in its new form is in accord with those of the interaction potential between a pair of protein monomers forming a lipid bilayer, in which the pairwise intermolecular potential is a function of the relative position of the two protein particles and the orientation of each of the particles. 47,53 As a consequence of the foregoing discussion, the net free-energy ψ b of the cylindrical body of the micelle can be expressed as ψb=true0L12(02πfalse(s,θfalse)0.2emnormaldθ)scriptDfalse(sfalse)0.2emnormalds, where the integrand of the inner integral, ( s , θ ), is false(s,θfalse)=true0L02π2trueΩfalse(1,2,3,4false)D(t)0.2emnormaldη0.2emnormaldt, with 1=ε2|boldχfalse(sfalse)boldχfalse(tfalse)|2, 2=boldχfalse(sfalse)boldχfalse(tfalse)false)·bolddfalse(s,θfalse), 3=boldχfalse(sfalse)boldχfalse(tfalse)false)·bolddfalse(t,ηfalse), and 4=bolddfalse(s,θfalse)·bolddfalse(t,ηfalse). Eq.…”
Section: Micro-mechanical Modelmentioning
confidence: 99%