Biophysical changes induced by cholesterol on phosphatidylcholine artificial biomembranes containing alamethicin oligomers

Cholesterol is an important constituent of eukaryotic cell membranes, whose interaction with phospholipids leads to a broad range of biological roles, such as: maintenance of proper fluidity, formation of raft domains, reduction of passive permeability of various chemical species through the bilayer (e.g., glucose, glycerol, K⁺, Na⁺ and Cl⁻ ions), and increased mechanical strength of the membrane. In this work we studied an interesting paradigm, as to whether cholesterol-containing phosphatidylcholine biomembranes influence the kinetics and transport features of alamethicin oligomers embedded into it. We demonstrate that moderate relative amounts of cholesterol increase the electrical conductance of various sub-conductance states of the alamethicin oligomer, caused probably by a non-monotonic change in the lumped dipole moment of the biomembrane. Our data suggest that biomembrane stiffness caused by cholesterol, visibly modifies the association-dissociation rates of alamethicin oligomerization in the biomembrane. Moreover, increasing concentrations of cholesterol seem to lead to more stable intermediate alamethicin oligomers. We show that in the presence of cholesterol, as the diameter of the alamethicin oligomer increases, so does the time of another monomer to get picked up. These results brings into focus the interesting issue of how oligomerization of proteins affects their interaction affinities for membrane-based lipids.     

Ion channels of N-terminally linked alamethicin dimers: enhancement of cation-selectivity by substitution of Glu for Gln at position 7

Alamethicin forms voltage-gated ion channels that have moderate cation-selectivity. The enhancement of the cation-selectivity by introducing negatively charged residues at positions 7 and 18 has been studied using the tethered homodimers of alamethicin with Q7 and E18 (di-alm-Q7E18) and its analog with E7 and Q18 (di-alm-E7Q18). In the dimeric peptides, monomer peptides are linked at the N-termini by a disulfide bond. Both the peptides formed long lasting ion channels at cis-positive voltages when added to the cis-side membrane. Their long open duration enabled us to obtain current-voltage (I-V(m)) relations and reversal potentials at the single-channel level by applying a voltage ramp during the channel opening. The reversal potentials measured in asymmetric KCl solutions indicated that ionized E7 provided strong cation-selectivity, whereas ionized E18 little influenced the charge selectivity. This was also the case for the macroscopic charge selectivity determined from the reversal potentials obtained by the macroscopic I-V(m) measurements. The results are accounted for by stronger electrostatic interactions between permeant ions and negatively charged residues at the narrowest part of the pore than at the pore mouth.     

Alamethicin–lipid interaction studied by energy dispersive X-ray diffraction

A detailed knowledge of the interaction between bacterial membranes and antibiotics provides important information to prevent high levels of antibiotic resistance exhibited by pathogenic strains. We investigated by energy dispersive X-ray diffraction (EDXD) the structure ordering of dioleoyl-phosphatidylcholine (DOPC) lipid interacting with antimicrobial peptide alamethicin, varying the lipid/peptide (L/P) molar ratio under two different hydration levels.In conditions of full hydration (100%) we found that the bilayer thickness is constant between L/P = 20 and L/P = 80 indicating that in this range, the system has reached the threshold value for the channel formation, while at the relative hydration of 45% a linear decrease of the bilayer thickness as function of L/P was revealed. The kinetic study of the complex alamethicin–DOPC at different L/P values, shows that the Bragg peak energy variation versus the hydration time has a biexponential behavior characterized by two different time constants.     

Analysis of the lipophilic peptaibol alamethicin by nonaqueous capillary electrophoresis-electrospray ionization-mass spectrometry

The microheterogeneous peptaibol alamethicin F30 isolated from the culture broth of Trichoderma viride was analyzed by nonaqueous CE-electrospray-MS using an IT and a TOF mass analyzer. Compared to aqueous buffers, higher separation selectivity was observed for methanolic BGE allowing the detection of more minor components. The low electrophoretic mobility observed for neutral analytes under nonaqueous conditions may be explained by ion-dipole interactions between the peptide analytes and electrolyte ions. The amino acid sequences of the individual components were derived from MS(n) using the doubly or triply charged pseudomolecular ions as well as characteristic fragments as precursor ions. The exchange of Ala by alpha-aminoisobutyric acid (Aib) which is frequently observed for peptaibols was detected for several components. Additional variations included the exchange of Gln to Glu, and the loss of the C-terminal amino alcohol or of the first six amino acids from the N-terminus with concomitant formation of pyroglutamyl residues. In most cases comigration of the Aib peptaibols with the respective Ala component was observed as the mass difference of 14 Da as the result of the amino acid exchange was not sufficient to translate into an electrophoretic separation under the conditions applied. However, proper selection of the precursor ions allowed the unequivocal analysis of the components. Additional TOF-MS measurements were performed in order to resolve the ammonium adducts from comigrating compounds (i.e., Aib-Ala exchange) and to confirm the amino acid composition of the individual components. Except for neutral compounds migrating close to the EOF the mass accuracy was better than 4 ppm for the doubly charged pseudomolecular ions and better than 2 ppm for triply charged ions.     

Extracting nucleation rates from current–time transients. Concluding remarks

Some time ago, Abyaneh and Fleischmann submitted several papers to this journal in which they modelled the heterogeneous nucleation of crystals as a first order kinetic process. In an invited response, I argued that such an approach was seriously flawed, because it ignored nucleation rate dispersion. More recently, instead of responding directly to this criticism, Abyaneh and Fleischmann have challenged the validity of the Deutscher–Fletcher experiments that first established the physical reality of nucleation rate dispersion. This note, therefore, serves two purposes. Firstly, it confirms the validity and high rigour of the original Deutscher–Fletcher experiments. Secondly, it identifies the errors in the Abyaneh–Fleischmann papers. In conclusion, it is emphasised that nucleation rate dispersion is real, universal, and must always be taken into account in experiments involving heterogeneous nucleation.