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. 2017 Mar 27;6:e22964. doi: 10.7554/eLife.22964

Figure 7. Free energy profiles for pore dilation, experimental results and model predictions.

The mathematical model describes a mechanism of pore expansion in which SNARE-crowding generates entropic expansion forces. (a) Open-pore free-energy landscape U(rpo) for different SNARE copy numbers. Increasing SNARE copy numbers in NLP discs softens the energy barrier against pore expansion. For vNLP30 discs, the profile starts rising above rpo7 nm (expected maximum size rpo, maxNLP78 nm). If a vesicle were fusing instead of a NLP, dilation would presumably relax pore curvature and lower the energy (dashed curve marked ‘vesicle’). vMSP data were obtained in earlier work (Wu et al., 2016) using smaller, ~16 nm diameter nanodiscs stabilized by the membrane scaffold protein (MSP), with 7–9 v-SNARE copies. The maximum allowable pore size is limited to slightly above the 2 nm radius of MSP discs. The same energy minimum around rpo0.5 nm is found regardless of copy numbers or the size of disc used, suggesting that this minimum represents an inherent property of fusing bilayers. (b) Corresponding free-energy profiles predicted by a mathematical model of the fusion pore with SNAREs (Materials and methods, Figure 7—figure supplement 1, and Table 1). Each curve shows the copy number and the net inward force (averaged over all pore sizes rpo>1.5 nm) tending to close down the pore to the minimum energy value. Membrane bending and tension resist pore expansion with a total force ~22 pN (SNARE-free pore, blue). In the presence of SNAREs, crowding effects produce an expansive entropic force that reduces the net inward force. The net force is progressively lowered with increasing numbers of SNAREs, reaching ~5 pN with 15 SNAREs. (c) Schematic illustrating a proposed SNARE-mediated pore expansion mechanism. Left: a few SNAREs can nucleate a pore, but dilation beyond a few nm is unlikely. Right: with many SNAREs, crowding generates expansion forces that are sufficient to offset the intrinsic bilayer resistance and to expand the pore. h,δ,D and ϕ are the height of the pore, the thickness of the membrane, the mean diameter of the vNLP discs, and the angle of twisting of the ApoE proteins, respectively. For definitions of other model parameters, see Materials and methods.

DOI: http://dx.doi.org/10.7554/eLife.22964.020

Figure 7.

Figure 7—figure supplement 1. Results of the mathematical model of the fusion pore in the presence of SNAREpins.

Figure 7—figure supplement 1.

(a) Membrane separation and angle of twist of the ApoE proteins versus pore size for a fusion pore without SNAREs. (b) Mean number of zippered SNAREs versus pore size for a fusion pore with N=0,2,4,7,15 total numbers of v-SNAREs per NLP face. (c) Free energy as a function of pore size and number of SNAREs (treated as a continuous variable).(d) Free energy as a function of pore size and membrane separation for fusion pores with N=1, 4, 15 total available v-SNAREs.