David P. Siegel

Energetics of intermediates in membrane fusion: comparison of stalk and inverted micellar intermediate mechanisms.

To understand the mechanism of membrane fusion, we have to infer the sequence of structural transformations that occurs during the process. Here, it is shown how one can estimate the lipid composition-dependent free energies of intermediate structures of different geometries. One can then infer which fusion mechanism is the best explanation of observed behavior in different systems by selecting the mechanism that requires the least energy. The treatment involves no adjustable parameters. It includes contributions to the intermediate energy resulting from the presence of hydrophobic interstices within structures formed between apposed bilayers. Results of these calculations show that a modified form of the stalk mechanism proposed by others is a likely fusion mechanism in a wide range of lipid compositions, but a mechanism based on inverted micellar intermediates (IMIs) is not. This should be true even in the vicinity of the lamellar/inverted hexagonal phase transition, where IMI formation would be most facile. Another prediction of the calculations is that traces of apolar lipids (e.g., long-chain alkanes) in membranes should have a substantial influence on fusion rates in general. The same theoretical methods can be used to generate and refine mechanisms for protein-mediated fusion.

The mechanism of lamellar-to-inverted hexagonal phase transitions in phosphatidylethanolamine: implications for membrane fusion mechanisms

We studied the mechanism of the lamellar-to-inverted hexagonal (L alpha/H[II]) phase transition, using time-resolved cryotransmission electron microscopy (TRC-TEM), 31P-NMR, and differential scanning calorimetry. The transition was initiated in dispersions of large unilamellar vesicles of dipalmitoleoyl phosphatidylethanolamine (DiPoPE). We present evidence that the transition proceeds in three steps. First, many small connections form between apposed membranes. Second, the connections aggregate within the planes of the bilayers, forming arrays with hexagonal order in some projections. Third, these quasihexagonal structures elongate into small domains of H(II) phase, acquiring lipid molecules by diffusion from contiguous bilayers. A previously proposed membrane fusion mechanism rationalizes these results. The modified stalk theory predicts that the L alpha/H(II) phase transition involves some of the same intermediate structures as membrane fusion. The small interbilayer connections observed via TRC-TEM are compatible with the structure of a critical intermediate in the modified stalk mechanism: the trans monolayer contact (TMC). The theory predicts that 1) TMCs should form starting at tens of degrees below TH; 2) when TMCs become sufficiently numerous, they should aggregate into transient arrays like the quasihexagonal arrays observed here by TRC-TEM; and 3) these quasihexagonal arrays can then elongate directly into H(II) phase domains. These predictions rationalize the principal features of our data, which are incompatible with the other transition mechanisms proposed to date. Thus these results support the modified stalk mechanism for both membrane fusion and the L alpha/H(II) phase transition. We also discuss some implications of the modified stalk theory for fusion in protein-containing systems. Specifically, we point out that recent data on the effects of hydrophobic peptides and viral fusion peptides on lipid phase behavior are consistent with an effect of the peptides on TMC stability.

Morphological Changes and Fusogenic Activity of Influenza Virus Hemagglutinin

The kinetics of low-pH induced fusion of influenza virus with liposomes have been compared to changes in the morphology of influenza hemagglutinin (HA). At pH 4.9 and 30 degrees C, the fusion of influenza A/PR/8/34 virus with ganglioside-bearing liposomes was complete within 6 min. Virus preincubated at pH 4.9 and 30 degrees C in the absence of liposomes for 2 or 10 min retained most of its fusion activity. However, fusion activity was dramatically reduced after 30 min, and virtually abolished after a 60-min preincubation. Cryo-electron microscopy showed that the hemagglutinin spikes of virions exposed to pH 4.9 at 30 degrees C for 10 min underwent no major morphological changes. After 30 min, however, the spike morphology changed dramatically, and further changes occurred for up to 60 min after exposure to low pH. Because the morphological changes occur at a rate corresponding to the loss of fusion activity, and because these changes are much slower than the rate at which fusion occurs, we conclude that the morphologically altered HA is inactive with respect to fusion-promoting activity. Molecular modeling studies indicate that the formation of an extended coiled coil within the HA trimer, as proposed for HA at low pH, requires a major conformational change in HA, and that the morphological changes we observe are consistent with the formation of an extended coiled coil. These results imply that the crystallographically determined low-pH form of HA does occur in the intact virus, but that this form is not a precursor of viral fusion. It is speculated that the motion to the low-pH form may be responsible for the membrane destabilization leading to fusion.

The Gaussian Curvature Elastic Energy of Intermediates in Membrane Fusion

The Gaussian curvature elastic energy contribution to the energy of membrane fusion intermediates has usually been neglected because the Gaussian curvature elastic modulus, kappa, was unknown. It is now possible to measure kappa for phospholipids that form bicontinuous inverted cubic (Q(II)) phases. Here, it is shown that one can estimate kappa for lipids that do not form Q(II) phases by studying the phase behavior of lipid mixtures. The method is used to estimate kappa for several lipid compositions in excess water. The values of kappa are used to compute the curvature elastic energies of stalks and catenoidal fusion pores according to recent models. The Gaussian curvature elastic contribution is positive and similar in magnitude to the bending energy contribution: it increases the total curvature energy of all the fusion intermediates by 100 units of k(B)T or more. It is important to note that this contribution makes the predicted intermediate energies compatible with observed lipid phase behavior in excess water. An order-of-magnitude fusion rate equation is used to estimate whether the predicted stalk energies are consistent with the observed rates of stalk-mediated processes in pure lipid systems. The current theory predicts a stalk energy that is slightly too large, by approximately 30 k(B)T, to rationalize the observed rates of stalk-mediated processes in phosphatidylethanolamine or N-monomethylated dioleoylphosphatidylethanolamine systems. Despite this discrepancy, the results show that models of fusion intermediate energy are accurate enough to make semiquantitative predictions about how proteins mediate biomembrane fusion. The same rate model shows that for proteins to drive biomembrane fusion at observed rates, they have to perform mediating functions corresponding to a reduction in the energy of a purely lipidic stalk by several tens of k(B)T. By binding particular peptide sequences to the monolayer surface, proteins could lower fusion intermediate energies by altering the elastic constants of the patches of lipid monolayer that form the stalk. Here, it is shown that if peptide binding changes kappa or some other combinations of local elastic constants by only tens of percents, the stalk energy and the energy of catenoidal fusion pores would decrease by tens of k(B)T relative to the pure lipid value. This is comparable to the required mediating effect. The curvature energies of stalks and catenoidal fusion pores have almost the same dependence on monolayer elastic constants as the curvature energies of the rhombohedral and Q(II) phases; respectively. The effects of isolated fusion-relevant peptides on the energies of these intermediates can be determined by studying the effects of the peptides on the stability of rhombohedral and Q(II) phases.

Membrane Fusion via Intermediates in Lα/HII Phase Transitions

Many researchers have suggested that membrane fusion can occur via structures that form during bilayer-to-non-bilayer phase transitions (for reviews, see [1–3]). These structures, detected via electron microscopy and 31P-NMR, were originally referred to as “lipidic particles” [4]. They seem to form between apposed lipid bilayers (generally in the “liquid crystalline”, or Lα phase) when conditions are such that the lipid is undergoing a phase transition to the inverted hexagonal (HII) phase, or is on the verge of doing so [1–3]. Such structures make the interfaces of apposed bilayers continuous, and this makes them attractive as postulated mediators of membrane fusion.