Fig. 7: Line tension λ of contact line between droplet and vesicle membrane as a function of lipid number Nol for three different droplet sizes Ddr, calculated via the force balance relationship in Eq. (12). | Nature Communications

Fig. 7: Line tension λ of contact line between droplet and vesicle membrane as a function of lipid number Nol for three different droplet sizes Ddr, calculated via the force balance relationship in Eq. (12).

From: Different pathways for engulfment and endocytosis of liquid droplets by nanovesicles

Fig. 7: Line tension λ of contact line between droplet and vesicle membrane as a function of lipid number Nol for three different droplet sizes Ddr, calculated via the force balance relationship in Eq. (12).The alternative text for this image may have been generated using AI.

As we increase Nol, which encodes the transbilayer asymmetry, the line tension undergoes a transition from positive to negative values. The line tension is positive for Nol = 5400 and 5500, for which the whole engulfment process remains axisymmetric and leads to neck cleavage and membrane fission. On the other hand, for Nol = 5700 and 5963, the line tension has a negative value and leads to the formation of a tight-lipped membrane neck as in Fig. 4 which prevents the fission process. The dashed vertical lines provide estimates for the lipid numbers \({N}_{{{\rm{ol}}}}={N}_{{{\rm{ol}}}}^{[0]}\) which lead to λ = 0 for the different droplet sizes Ddr. The numerical values of \({N}_{{{\rm{ol}}}}^{[0]}\), which depend on the droplet size, are given in the last column of Table 1. Each red, green, and blue data point represents the mean value over n = 15 statistically independent samples obtained from three replicated simulations. Each error bar is the SEM.

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