Abstract:The lateral membrane organization and phase behavior of the binary lipid mixture DMPC (1,2-dimyristoyl-sn-glycero-3-phosphatidylcholine) - DSPC (1,2-distearoyl-sn-glycero-3-phosphatidylcholine) without and with incorporated gramicidin D (GD) as a model biomembrane polypeptide was studied by small-angle neutron scattering, Fourier-transform infrared spectroscopy, and by two-photon excitation fluorescence microscopy on giant unilamellar vesicles. The small-angle neutron scattering method allows the detection of … Show more
“…Indeed, in this region we expect the two lipids to be mostly segregated into DSPC gel domains and DMPC fluid domains (40,41). From our previous results, we expect only the fluid DMPC domain fluctuations to be measurable and their amplitude to be z0.4 nm, which matches the amplitude measured in this coexistence region within the experimental error.…”
Membrane thickness fluctuations have been associated with a variety of critical membrane phenomena, such as cellular exchange, pore formation, and protein binding, which are intimately related to cell functionality and effective pharmaceuticals. Therefore, understanding how these fluctuations are controlled can remarkably impact medical applications involving selective macromolecule binding and efficient cellular drug intake. Interestingly, previous reports on single-component bilayers show almost identical thickness fluctuation patterns for all investigated lipid tail-lengths, with similar temperature-independent membrane thickness fluctuation amplitude in the fluid phase and a rapid suppression of fluctuations upon transition to the gel phase. Presumably, in vivo functions require a tunability of these parameters, suggesting that more complex model systems are necessary. In this study, we explore lipid tail-length mismatch as a regulator for membrane fluctuations. Unilamellar vesicles of an equimolar mixture of dimyristoylphosphatidylcholine and distearoylphosphatidylcholine molecules, with different tail-lengths and melting transition temperatures, are used as a model system for this next level of complexity. Indeed, this binary system exhibits a significant response of membrane dynamics to thermal variations. The system also suggests a decoupling of the amplitude and the relaxation time of the membrane thickness fluctuations, implying a potential for independent control of these two key parameters.
“…Indeed, in this region we expect the two lipids to be mostly segregated into DSPC gel domains and DMPC fluid domains (40,41). From our previous results, we expect only the fluid DMPC domain fluctuations to be measurable and their amplitude to be z0.4 nm, which matches the amplitude measured in this coexistence region within the experimental error.…”
Membrane thickness fluctuations have been associated with a variety of critical membrane phenomena, such as cellular exchange, pore formation, and protein binding, which are intimately related to cell functionality and effective pharmaceuticals. Therefore, understanding how these fluctuations are controlled can remarkably impact medical applications involving selective macromolecule binding and efficient cellular drug intake. Interestingly, previous reports on single-component bilayers show almost identical thickness fluctuation patterns for all investigated lipid tail-lengths, with similar temperature-independent membrane thickness fluctuation amplitude in the fluid phase and a rapid suppression of fluctuations upon transition to the gel phase. Presumably, in vivo functions require a tunability of these parameters, suggesting that more complex model systems are necessary. In this study, we explore lipid tail-length mismatch as a regulator for membrane fluctuations. Unilamellar vesicles of an equimolar mixture of dimyristoylphosphatidylcholine and distearoylphosphatidylcholine molecules, with different tail-lengths and melting transition temperatures, are used as a model system for this next level of complexity. Indeed, this binary system exhibits a significant response of membrane dynamics to thermal variations. The system also suggests a decoupling of the amplitude and the relaxation time of the membrane thickness fluctuations, implying a potential for independent control of these two key parameters.
“…A b 5.6 -helix consisting of twelve amino acids with a pitch of 5.1 would exhibit a length of approximately 29 while the corresponding b 6.3 -helix with a 3.3 pitch would feature a length of approximately 21 . [46][47][48][49][50] Considering these facts in addition to the CD results and previous studies, the distance indicated in the electron density difference curves by the major peaks that are located right beneath the lipid head-groups additionally suggest the existence of a membrane-spanning b 5.6 -helix. Especially because of the recently reported crystal structure where the peptides of the present motif seem to be slightly shorter than the typical b 5.6 -helical structure, maybe due to the steric effects of the side chains and by means of hydrophobic mismatch an extension of the considered species of 0.8 is highly reasonable.…”
Section: Membrane Incorporation Of B 56 -Helices and X-ray Reflectivitysupporting
Structural parameters, such as conformation, orientation and penetration depth of membrane-bound peptides and proteins that may function as channels, pores or biocatalysts, are of persistent interest and have to be probed in the native fluid state of a membrane. X-ray scattering in combination with heavy-atom labeling is a powerful and highly appropriate method to reveal the position of a certain amino acid residue within a lipid bilayer with respect to the membrane normal axis up to a resolution of several Angstrøm. Herein, we report the synthesis of a new iodine-labeled amino acid building block. This building block is intended for peptide incorporation to provide high intensities for electron density difference analysis of X-ray reflectivity data and improve the labeling potential for the lipid bilayer head-group and water region. The novel building block as well as the commercially available non-iodinated analogue, required for X-ray scattering, was implemented in a transmembrane peptide motif via manual solid-phase peptide synthesis (SPPS) following the fluorenylmethyloxycarbonyl (Fmoc)-strategy. The derived peptides were reconstituted in lipid vesicles as well as in highly aligned multilamellar lipid stacks and investigated via circular dichroism (CD) and X-ray reflectivity. Thereby, it has been revealed that the bulky iodine probe neither causes conformational change of the peptide structure nor lamellar disordering of the membrane complexes.
“…The circular shape of the domains observed here ( Figure 5B), which contrasts with the gel-fluid type domains seen in Figure 2, is typical for minimizing the area-to-perimeter ratio for isotropic phases in equilibrium. This kind of shape is also observed in model raft mixtures 42 that are thought to consist of liquid-ordered/liquid-disordered domains. These findings can be explained by a lipid sorting mechanism and phase separation on the vesicle surface induced by the polypeptide.…”
Section: Discussionsupporting
confidence: 55%
“…11 Recently, we studied giant unilamellar vesicles (GUVs) of the pure lipid mixture using two different fluorophores (Laurdan and N-Rh-DPPE) in two-photon excitation fluorescence microscopy studies. 42 In the case of N-Rh-DPPE, the different probe partitioning between gel and fluid domains discriminates between fluid and gel-state domains. In the fluid phase of the lipid bilayer system, at T g 49°C, the images obtained with N-Rh-DPPE as fluorophor show that the fluorescent molecules are distributed homogeneously on the vesicle surface ( Figure 2).…”
Abstract:The lateral membrane organization and phase behavior of the lipid mixture DMPC(di-C14)/DSPC-(di-C18)/cholesterol (0-33 mol %) with and without an incorporated fluorescence-labeled palmitoyl/farnesyl dual-lipidated peptide, BODIPY-Gly-Cys(Pal)-Met-Gly-Leu-Pro-Cys(Far)-OMe, which represents a membrane recognition model system for Ras proteins, was studied by two-photon excitation fluorescence microscopy. Measurements were performed on giant unilamellar vesicles (GUVs) over a large temperature range, ranging from 30 to 80°C to cover different lipid phase states (all-gel, fluid/gel, liquid-ordered, all-fluid). At temperatures where the fluid-gel coexistence region of the pure binary phospholipid system occurs, large-scale concentration fluctuations appear. Incorporation of cholesterol levels up to 33 mol % leads to a significant increase of conformational order in the membrane system and a reduction of large domain structures. Adding the peptide leads to dramatic changes in the lateral organization of the membrane. With cholesterol present, a phase separation is induced by a lipid sorting mechanism owing to the high affinity of the lipidated peptide to a fluid, DMPC-rich environment. This phase separation leads to the formation of peptide-containing domains with high fluorescence intensity that become progressively smaller with decreasing temperature. As a result, the local concentration of the peptide increases steadily within the confines of the shrinking domains. At the lowest temperatures, where the acyl-chain order parameter of the membrane has already drastically increased and the membrane achieves a liquid-ordered character, an efficient lipid sorting mechanism is no longer supported and aggregation of the peptide into small clusters prevails. We can conclude that palmitoyl/farnesyl dual-lipidated peptides do not associate with liquid-ordered or gel-like domains in phase-separated bilayer membranes. In particular, the study shows the interesting ability of the peptide to induce formation of fluid microdomains at physiologically relevant cholesterol concentrations, and this effect very much depends on the concentration of fluid vs ordered lipid molecules.
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