Interaction of phospholipids with proteins and peptides. New advances III

New user-friendly approach to obtain an Eisenberg plot and its use as a practical tool in protein sequence analysis

The Eisenberg plot or hydrophobic moment plot methodology is one of the most frequently used methods of bioinformatics. Bioinformatics is more and more recognized as a helpful tool in Life Sciences in general, and recent developments in approaches recognizing lipid binding regions in proteins are promising in this respect. In this study a bioinformatics approach specialized in identifying lipid binding helical regions in proteins was used to obtain an Eisenberg plot. The validity of the Heliquest generated hydrophobic moment plot was checked and exemplified. This study indicates that the Eisenberg plot methodology can be transferred to another hydrophobicity scale and renders a user-friendly approach which can be utilized in routine checks in protein–lipid interaction and in protein and peptide lipid binding characterization studies. A combined approach seems to be advantageous and results in a powerful tool in the search of helical lipid-binding regions in proteins and peptides. The strength and limitations of the Eisenberg plot approach itself are discussed as well. The presented approach not only leads to a better understanding of the nature of the protein–lipid interactions but also provides a user-friendly tool for the search of lipid-binding regions in proteins and peptides.

Stability and state of aggregation of aqueous fibrinogen and dipalmitoylphosphatidylcholine lipid vesicles

The stability and state of aggregation of aqueous fibrinogen (FB) and dipalmitoylphosphatidylcholine (DPPC) vesicles in water or buffer at 25 degrees C were studied with dynamic light scattering (DLS), UV-vis spectroturbidimetry (ST), and cryo-transmission electron microscopy (cryo-TEM). In water, when 1000 ppm (0.10 wt %) DPPC dispersions were prepared with a protocol including extensive sonication, they contained mostly vesicles and were quite clear, transparent, and stable for at least 30 days. FB mixtures with water (0.075 wt %) were quite unstable and biphasic. They formed large aggregates which eventually precipitated. The addition of DPPC vesicles into these unstable FB dispersions reversed FB aggregation and precipitation and produced stable translucent microdispersions. The inferred lipid/protein aggregates were limited in size, with average diameters ranging from 200 to 300 nm. In buffer, DPPC dispersions were also clear and quite stable, with average dispersed particles diameter of ca. 90 nm. FB dissolved in aqueous buffer and formed transparent and stable solutions. Adding salt to an aggregated FB dispersion in water reversed the aggregation. FB aggregated and redissolved in the presence of the citrate and after the citrate was removed. There was no effect of citrate (present in FB initially) in the FB aggregation or redissolution. FB molecules in buffer form dimers or higher aggregates. Their average aggregation number is 2, determined with Rayleigh scattering analysis of turbidity data. The average hydrodynamic diameter of FB solutions from DLS was 30 nm. Mixing a stable FB solution in buffer and a stable DPPC dispersion in buffer produced highly unstable mixtures, in which large aggregates precipitated. These results have implications in understanding the interactions of lipids and proteins in many biological applications and food processing applications.

Interaction of a peptide model of a hydrophobic transmembrane alpha-helical segment of a membrane protein with phosphatidylethanolamine bilayers: differential scanning calorimetric and Fourier transform infrared spectroscopic studies

High-sensitivity differential scanning calorimetry (DSC) and Fourier transform infrared (FTIR) spectroscopy were used to study the interaction of a synthetic alpha-helical hydrophobic transmembrane peptide, Acetyl-Lys2-Gly-Leu24-Lys2-Ala-Amide, and members of a homologous series of n-saturated diacylphosphatidylethanolamines (PEs). In the lower range of peptide mol fractions, the DSC endotherms exhibited by the lipid/peptide mixtures consist of two components. The temperature and cooperativity of the sharper, higher-temperature component are very similar to those of pure PE bilayers and are almost unaffected by variations in the peptide/lipid ratio. However, the fractional contribution of this component to the total enthalpy change decreases with increases in peptide concentration, and this component completely disappears at higher peptide mol fractions. The other component, which is less cooperative and occurs at a lower temperature, predominates at higher peptide concentrations. These two components of the DSC endotherm can be attributed to the chain-melting phase transitions of peptide-nonassociated and peptide-associated PE molecules, respectively. Although the temperature at which the peptide-associated PE molecules melt is progressively decreased by increases in peptide concentration, the magnitude of this shift is independent of the length of the PE hydrocarbon chain. In addition, the width of the phase transition observed at higher peptide concentrations is also relatively insensitive to PE hydrocarbon chain length, except that peptide gel-phase immiscibility occurs in very short- or very long-chain PE bilayers. Moreover, the enthalpy of the chain-melting transition of the peptide-associated PE does not decrease to 0 even at high peptide concentrations, suggesting that this peptide does not abolish the cooperative gel/liquid-crystalline phase transition of the lipids with which it is in contact. The FTIR spectroscopic data indicate that the peptide remains in a predominantly alpha-helical conformation, but that the peptide alpha-helix is subject to small distortions coincident with the changes in hydrophobic thickness that accompany the chain-melting phase transition of the PE bilayer. These data also indicate that the peptide significantly disorders the hydrocarbon chains of adjacent PE molecules in both the gel and liquid-crystalline states relatively independently of lipid hydrocarbon chain length. The relative independence of many aspects of PE-peptide interactions on the hydrophobic thickness of the host bilayer observed in the present study is in marked contrast to the results of our previous study of peptide-phosphatidylcholine (PC) model membranes (Zhang et al. (1992) Biochemistry 31:11579-11588), where strong hydrocarbon chain length-dependent effects were observed. The differing effects of peptide incorporation on PE and PC bilayers is ascribed to the much stronger lipid polar headgroup interactions in the former system. We postulate that the primary effect of transmembrane peptide incorporation into PE bilayers is the disruption of the relatively strong electrostatic and hydrogen-bonding interactions at the bilayer surface, and that this effect is sufficiently large to mask the effect of hydrophobic mismatch between the lengths of the hydrophobic core of the peptide and its host bilayer.