Effect of Transmembrane Asymmetric Distribution of Lipids and Peptides on Lipid Bilayers.

The transbilayer asymmetry of the biomembrane is generated due to the differences in lipid and protein compositions between two leaflets, which plays important roles in physiological functions. However, transbilayer asymmetry can also be originated due to a nonequal number of lipids or proteins in each leaflet, which has not been well recognized. Therefore, to shed light on this field, here we generated theoretical models for the effect of transbilayer asymmetry originated from the differences in the number of lipids and peptides in each leaflet on the state of lipid bilayers. The first model described the effect of asymmetric lipid distribution on the state of lipid bilayers. We obtained theoretical equations for the fractional change in area per lipid in both leaflets as a function of the ratio of the number of lipids in each leaflet, which agreed with the molecular dynamics simulation results quantitatively. Results indicated that tensions in both leaflets are opposite in direction, and their magnitude is the same. We also performed experiments on the effect of lipid insertion in the outer leaflet on the fractional change in area per lipid. These results agreed quantitatively with the values predicted by the above model. The second model described the effect of asymmetric distribution of peptides on the state of lipid bilayers. We obtained theoretical equations for the area per lipid in both leaflets as a function of the surface concentration of peptides located only in the outer leaflet, which agreed with the results of the antimicrobial peptide magainin 2-induced area change.

Mechanism of Initial Stage of Pore Formation Induced by Antimicrobial Peptide Magainin 2.

Antimicrobial peptide magainin 2 forms pores in lipid bilayers, a property that is considered the main cause of its bactericidal activity. Recent data suggest that tension or stretching of the inner monolayer plays an important role in magainin 2-induced pore formation in lipid bilayers. Here, to elucidate the mechanism of magainin 2-induced pore formation, we investigated the effect on pore formation of asymmetric lipid distribution in two monolayers. First, we developed a method to prepare giant unilamellar vesicles (GUVs) composed of dioleoylphosphatidylglycerol (DOPG), dioleoylphosphatidylcholine (DOPC), and lyso-PC (LPC) in the inner monolayer and of DOPG/DOPC in the outer monolayer. We consider that in these GUVs, the lipid packing in the inner monolayer was larger than that in the outer monolayer. Next, we investigated the interaction of magainin 2 with these GUVs with an asymmetric distribution of LPC using the single GUV method, and found that the rate constant of magainin 2-induced pore formation, kp, decreased with increasing LPC concentration in the inner monolayer. We constructed a quantitative model of magainin 2-induced pore formation, whereby the binding of magainin 2 to the outer monolayer of a GUV induces stretching of the inner monolayer, causing pore formation. A theoretical equation defining kp as a function of magainin 2 surface concentration, X, reasonably explains the experimental relationship between kp and X. This model quantitatively explains the effect on kp of the LPC concentration in the inner monolayer. On the basis of these results, we discuss the mechanism of the initial stage of magainin 2-induced pore formation.

Continuous detection of entry of cell-penetrating peptide transportan 10 into single vesicles.

Entry of cell-penetrating peptides (CPPs) into living cells by translocating across plasma membranes is an important physiological phenomenon. To elucidate the mechanism of the translocation of CPPs across lipid bilayers, it is essential to reveal its elementary processes. For this purpose, here, we have developed a new method for the continuous, quantitative detection of the entry of CPPs into giant unilamellar vesicles (GUVs), where we investigate the interaction of fluorescent probe-labeled CPPs with single GUVs containing large unilamellar vesicles (LUVs) and fluorescent probes in their lumens using confocal microscopy. Using this method, we investigated the interaction of carboxyfluorescein (CF)-labeled transportan 10 (CF-TP10) with single GUVs comprised of dioleoylphosphatidylglycerol (DOPG) and dioleoylphosphatidylcholine (DOPC) containing LUVs of the same membrane and Alexa Fluor 647 hydrazide (AF647) in their lumens. At low concentrations of CF-TP10, first the fluorescence intensity (FI) of the GUV membrane increased with time, and then after some lag time the FI of the GUV lumen due to CF-TP10 increased continuously with time without leakage of AF647. At higher concentrations of CF-TP10, after the FI of the GUV lumen due to CF-TP10 increased significantly, leakage of AF647 started. These results indicate that CF-TP10 entered the GUV lumen by translocating across the GUV membrane and then bound to the LUVs there without pore formation and that CF-TP10 concentration in the lumen increased with time. The rate of entry of CF-TP10 into GUV lumen increased with CF-TP10 concentration. We discussed the kinetics of entry of CF-TP10 into single GUVs.

Effects of Mechanical Properties of Lipid Bilayers on the Entry of Cell-Penetrating Peptides into Single Vesicles.

The translocation of cell-penetrating peptides (CPPs) through plasma membranes of living cells is an important physiological phenomenon in biomembranes. To reveal the mechanism underlying the translocation of a CPP, transportan 10 (TP10), through lipid bilayers, we examined the effects of the mechanical properties of lipid bilayers on the entry of carboxyfluorescein (CF)-labeled TP10 (CF-TP10) into a giant unilamellar vesicle (GUV) using the single GUV method. First, we examined the effect of lateral tension in membranes on the entry of CF-TP10 into single GUVs comprising a mixture of dioleoylphosphatidylglycerol (DOPG) and dioleoylphosphatidylcholine (DOPC) (2/8). CF-TP10 entered the GUV lumen before the membrane permeation of Alexa Fluor 647 hydrazide (AF647) from the GUV and thus before pore formation in the membrane. The fraction of entry of CF-TP10 before pore formation and the rate of membrane rupture increased with tension. The CF-TP10-induced fractional change in the membrane area increased continuously with time until membrane rupture, but it increased more slowly than did the CF-TP10 concentration in the GUV membrane. A high mole fraction of cholesterol inhibited the entry of CF-TP10 into single GUVs by suppressing the translocation of CF-TP10 from the external to the internal monolayer, although higher concentrations of CF-TP10 induced the formation of pores through which CF-TP10 rapidly translocated. Suppression of the translocation of CF-TP10 by cholesterol can be reasonably explained by the large line tension of a prepore. We discussed the role of mechanical properties in membranes on the entry of CF-TP10 into single GUVs and proposed a hypothesis of the mechanism that CF-TP10 translocates across a bilayer through transient hydrophilic prepores in the membrane.

Analysis of constant tension-induced rupture of lipid membranes using activation energy.

The stretching of biomembranes and lipid membranes plays important roles in various physiological and physicochemical phenomena. Here we analyzed the rate constant kp of constant tension-induced rupture of giant unilamellar vesicles (GUVs) as a function of tension σ using their activation energy Ua. To determine the values of kp, we applied constant tension to a GUV membrane using the micropipette aspiration method and observed the rupture of GUVs, and then analyzed these data statistically. First, we investigated the temperature dependence of kp for GUVs of charged lipid membranes composed of negatively charged dioleoylphosphatidylglycerol (DOPG) and electrically neutral dioleoylphosphatidylcholine (DOPC). By analyzing this result, the values of Ua of tension-induced rupture of DOPG/DOPC-GUVs were obtained. Ua decreased with an increase in σ, supporting the classical theory of tension-induced pore formation. The analysis of the relationship between Ua and σ using the theory on the electrostatic interaction effects on the tension-induced rupture of GUVs provided the equation of Ua including electrostatic interaction effects, which well fits the experimental data of the tension dependence of Ua. A constant which does not depend on tension, U0, was also found to contribute significantly to Ua. The Arrhenius equations for kp using the equation of Ua and the parameters determined by the above analysis fit well to the experimental data of the tension dependence of kp for DOPG/DOPC-GUVs as well as for DOPC-GUVs. On the basis of these results, we discussed the possible elementary processes underlying the tension-induced rupture of GUVs of lipid membranes. These results indicate that the Arrhenius equation using the experimentally determined Ua is useful in the analysis of tension-induced rupture of GUVs.

Electrostatic interaction effects on tension-induced pore formation in lipid membranes.

We investigated the effects of electrostatic interactions on the rate constant (k(p)) for tension-induced pore formation in lipid membranes of giant unilamellar vesicles under constant applied tension. A decrease in salt concentration in solution as well as an increase in surface charge density of the membranes increased k(p). These data indicate that k(p) increases as the extent of electrostatic interaction increases. We developed a theory on the effect of the electrostatic interactions on the free energy profile of the membrane containing a prepore and also on the values of k(p); this theory explains the experimental results and fits the experimental data reasonably well in the presence of weak electrostatic interactions. Based on these results, we conclude that a decrease in the free energy barrier of the prepore state due to electrostatic interactions is the main factor causing an increase in k(p).