Spin-label electron spin resonance and Fourier transform infrared spectroscopy for structural/dynamic measurements on ion channels

Salt-Induced Membrane-Bound Conformation of the NAC Domain of α-Synuclein Leads to Structural Polymorphism of Amyloid Fibrils

α-Synuclein (αS) interacts with lipid membranes in neurons to form amyloid fibrils that contribute to Parkinson's disease, and its non-amyloid-β component domain is critical in the fibrillation. In this study, the salt (NaCl) effect on the membrane interaction and fibril formation of αS57-102 peptide (containing the non-amyloid-β component domain) was characterized at the molecular level because the αS57-102 fibrils exhibited structural polymorphism with two morphologies (thin and thick) in the presence of NaCl but showed one morphology (thin) in the absence of NaCl. The membrane-bound conformation (before fibrillation) of αS57-102 had two helical regions (first and second) on the membrane regardless of salt, but the length of the first region largely shortened when NaCl was present, exposing its hydrophobic area to the solvent. The exposed region induced two distinct pathways of fibril nucleation, depending on the molar ratios of free and membrane-bound αS57-102: one from the association of free αS57-102 with membrane-bound αS57-102 and the other from the assembly among membrane-bound αS57-102. The differences mainly affected the β-strand orientation and helical content within the fibril conformations, probably contributing to the thickness degree, leading to structural polymorphism.

Interaction of Vitamin K1 and Vitamin K2 with Dimyristoylphosphatidylcholine and Their Location in the Membrane

Vitamin K₁ and vitamin K₂ play very important biological roles as members of chains of electron transport as antioxidants in membranes and as cofactors for the posttranslational modification of proteins that participate in a number of physiological functions such as coagulation. The interaction of these vitamins with dimyristoylphosphatidylcholine (DMPC) model membranes has been studied by using a biophysical approach. It was observed by using differential scanning calorimetry that both vitamins have a very limited miscibility with DMPC and they form domains rich in the vitamins at high concentrations. Experiments using X-ray diffraction also showed the formation of different phases as a consequence of the inclusion of either vitamin K at temperatures below the phase transition. However, in the fluid state, a homogeneous phase was detected, and a decrease in the thickness of the membrane was accompanied by an increase in the water layer thickness. ²H NMR spectroscopy showed that both vitamins K induced a decrease in the onset of the phase transition, which was bigger for vitamin K₁, and both vitamins decreased the order of the membrane as seen through the first moment (M₁). ¹H NOESY MAS-NMR showed that protons located at the rings or at the beginning of the lateral chain of both vitamins K interacted with a clear preference with protons located in the polar part of DMPC. On the other hand, protons located on the lateral chain have a nearer proximity with the methyl end of the myristoyl chains of DMPC. In agreement with the ²H NMR, ATR-FTIR (attenuated total reflectance Fourier transform infrared spectroscopy) indicated that both vitamins decreased the order parameters of DMPC. It was additionally deduced that the lateral chains of both vitamins were oriented almost in parallel to the myristoyl chains of the phospholipid.

Phenolic Group of α-Tocopherol Anchors at the Lipid-Water Interface of Fully Saturated Membranes

α-Tocopherol is considered to carry on a very important role as an antioxidant for membranes and lipoproteins and other biological roles as membrane stabilizers and bioactive lipids. Given its essential role, it is very important to fully understand its location in the membrane. In this work, the vertical location of vitamin E in saturated membranes has been studied using biophysical techniques. Small- and wide-angle X-ray diffraction experiments show that α-tocopherol alters the water layer between bilayers in both 1,2-dimyristoyl- sn-glycero-3-phosphocholine (DMPC) and 1,2-dipalmitoyl- sn-glycero-3-phosphocholine (DPPC), indicating its proximity to this surface. The quenching of the intrinsic fluorescence of α-tocopherol indicates a low quenching efficiency by acrylamide and a higher quenching by 5-doxyl-PC than by 9- and 16-doxyl-PC. These results suggest that in both DMPC and DPPC membranes, the chromanol ring is not far away from the surface of the membrane but within the bilayer. ¹H nuclear Overhauser enhancement spectroscopy magic-angle spinning-nuclear magnetic resonance studies showed that α-tocopherol is localized in a similar manner in DMPC and DPPC membranes, with the chromanol ring embedded in the upper part of the hydrophobic bilayer. Using attenuated total reflection-Fourier transform infrared spectroscopy, it was observed that the tail chain of α-tocopherol lies nearly parallel to the acyl chains of DMPC and DPPC. Taking these results together, it was concluded that in both DMPC and DPPC, the hydroxyl group of the chromanol ring will establish hydrogen bonding with water on the membrane surface, and the main axis of the α-tocopherol molecule will be perpendicular to the bilayer plane.

Membrane docking of the C2 domain from protein kinase Cα as seen by polarized ATR-IR. The role of PIP₂

We have used attenuated total internal reflection infrared spectroscopy (ATR-IR) spectroscopy to study the association of the C2 domain from protein kinase Cα (PKCα) with different phospholipid membranes, so as to characterise the mode of membrane docking and its modulation by the second-messenger lipid PIP₂. In parallel, we have also examined the membrane interaction of the C2 domain from cytosolic phospholipase A₂. PIP₂ did not induce significant changes in secondary structure of the membrane-bound PKCα-C2 domain, nor did binding of the PKCα-C2 domain change the dichroic ratios of the lipid chains, whereas the C2 domain from phospholipase A₂ did perturb the lipid chain orientation. Measurements of the dichroic ratios for the amide I and amide II protein bands were combined so as to distinguish the tilt of the β-sheets from that of the β-strands within the sheet. When associated with POPC/POPS membranes, the β-sandwich of the PKCα-C2 domain is inclined at an angle α=35° to the membrane normal, i.e., is oriented more nearly perpendicular than parallel to the membrane. In the process of membrane docking, the tilt angle increases to α=44° in the presence of PIP₂, indicating that the β-sandwich comes closer to the membrane surface, so confirming the importance of this lipid in determining docking of the C2 domain and consequent activation of PKCα.

Orientation determination of interfacial beta-sheet structures in situ

Structural information such as orientations of interfacial proteins and peptides is important for understanding properties and functions of such biological molecules, which play crucial roles in biological applications and processes such as antimicrobial selectivity, membrane protein activity, biocompatibility, and biosensing performance. The alpha-helical and beta-sheet structures are the most widely encountered secondary structures in peptides and proteins. In this paper, for the first time, a method to quantify the orientation of the interfacial beta-sheet structure using a combined attenuated total reflectance Fourier transformation infrared spectroscopic (ATR-FTIR) and sum frequency generation (SFG) vibrational spectroscopic study was developed. As an illustration of the methodology, the orientation of tachyplesin I, a 17 amino acid peptide with an antiparallel beta-sheet, adsorbed to polymer surfaces as well as associated with a lipid bilayer was determined using the regular and chiral SFG spectra, together with polarized ATR-FTIR amide I signals. Both the tilt angle (theta) and the twist angle (psi) of the beta-sheet at interfaces are determined. The developed method in this paper can be used to obtain in situ structural information of beta-sheet components in complex molecules. The combination of this method and the existing methodology that is currently used to investigate alpha-helical structures will greatly broaden the application of optical spectroscopy in physical chemistry, biochemistry, biophysics, and structural biology.

Orientation determination of protein helical secondary structures using linear and nonlinear vibrational spectroscopy

In this paper, we systematically presented the orientation determination of protein helical secondary structures using vibrational spectroscopic methods, particularly, nonlinear sum frequency generation (SFG) vibrational spectroscopy, along with linear vibrational spectroscopic techniques such as infrared spectroscopy and Raman scattering. SFG amide I signals can be collected using different polarization combinations of the input laser beams and output signal beam to measure the second-order nonlinear optical susceptibility components of the helical amide I modes, which are related to their molecular hyperpolarizability elements through the orientation distribution of these helices. The molecular hyperpolarizability elements of amide I modes of a helix can be calculated based on the infrared transition dipole moment and Raman polarizability tensor of the helix; these quantities are determined by using the bond additivity model to sum over the individual infrared transition dipole moments and Raman polarizability tensors, respectively, of the peptide units (or the amino acid residues). The computed overall infrared transition dipole moment and Raman polarizability tensor of a helix can be validated by experimental data using polarized infrared and polarized Raman spectroscopy on samples with well-aligned helical structures. From the deduced SFG hyperpolarizability elements and measured SFG second-order nonlinear susceptibility components, orientation information regarding helical structures can be determined. Even though such orientation information can also be measured using polarized infrared or polarized Raman amide I signals, SFG has a much lower detection limit, which can be used to study the orientation of a helix when its surface coverage is much lower than a monolayer. In addition, the combination of different vibrational spectroscopic techniques, for example, SFG and attenuated total reflectance Fourier transform infrared spectroscopy, provides more measured parameters for orientation determination, aiding in the deduction of more complicated orientation distributions. In this paper, we discussed two types of helices, the alpha-helix and 3-10 helix. However, the orientation determination method presented here is general and thus can be applied to study other helices as well. The calculations of SFG amide I hyperpolarizability components for alpha-helical and 3-10 helical structures with different chain lengths have also been performed. It was found that when the helices reached a certain length, the number of peptide units in the helix should not alter the data analysis substantially. It was shown in the calculation, however, that when the helix chain is short, the SFG hyperpolarizability component ratios can vary substantially when the chain length is changed. Because 3-10 helical structures can be quite short in proteins, the orientation determination for a short 3-10 helix needs to take into account the number of peptide units in the helix.

Protein-lipid interactions with Fusobacterium nucleatum major outer membrane protein FomA: spin-label EPR and polarized infrared spectroscopy

FomA, the major outer membrane protein of Fusobacterium nucleatum, was expressed and purified in Escherichia coli and reconstituted from detergent in bilayer membranes of phosphatidylcholines with chain lengths from C(12:0) to C(17:0). The conformation and orientation of membrane-incorporated FomA were determined from polarized, attenuated total reflection, infrared (IR) spectroscopy, and lipid-protein interactions with FomA were characterized by using electron paramagnetic resonance (EPR) spectroscopy of spin-labeled lipids. Approximately 190 residues of membranous FomA are estimated to be in a beta-sheet configuration from IR band fitting, which is consistent with a 14-strand transmembrane beta-barrel structure. IR dichroism of FomA indicates that the beta-strands are tilted by approximately 45 degrees relative to the sheet/barrel axis and that the order parameter of the latter displays a discontinuity corresponding to hydrophobic matching with fluid C(13:0) lipid chains. The stoichiometry ( N b = 23 lipids/monomer) of lipid-protein interaction from EPR demonstrates that FomA is not trimeric in membranes of diC(14:0) phosphatidylcholine and is consistent with a monomeric beta-barrel of 14-16 strands. The pronounced selectivity of interaction found with anionic spin-labeled lipids places basic residues of the protein in the vicinity of the polar-apolar membrane interfaces, consistent with current topology models. Comparison with similar data from the 8- to 22-stranded E. coli outer membrane proteins, OmpA, OmpG, and FhuA, supports the above conclusions.

Incorporation of outer membrane protein OmpG in lipid membranes: protein-lipid interactions and beta-barrel orientation

OmpG is an intermediate size, monomeric, outer membrane protein from Escherichia coli, with n beta = 14 beta-strands. It has a large pore that is amenable to modification by protein engineering. The stoichiometry ( N b = 20) and selectivity ( K r = 0.7-1.2) of lipid-protein interaction with OmpG incorporated in dimyristoyl phosphatidylcholine bilayer membranes was determined with various 14-position spin-labeled lipids by using EPR spectroscopy. The limited selectivity for different lipid species is consistent with the disposition of charged residues in the protein. The conformation and orientation (beta-strand tilt and beta-barrel order parameters) of OmpG in disaturated phosphatidylcholines of odd and even chain lengths from C(12:0) to C(17:0) was determined from polarized infrared spectroscopy of the amide I and amide II bands. A discontinuity in the protein orientation (deduced from the beta-barrel order parameters) is observed at the point of hydrophobic matching of the protein with lipid chain length. Compared with smaller (OmpA; n beta = 8) and larger (FhuA; n beta = 22) monomeric E. coli outer membrane proteins, the stoichiometry of motionally restricted lipids increases linearly with the number of beta-strands, the tilt (beta approximately 44 degrees ) of the beta-strands is comparable for the three proteins, and the order parameter of the beta-barrel increases regularly with n beta. These systematic features of the integration of monomeric beta-barrel proteins in lipid membranes could be useful for characterizing outer membrane proteins of unknown structure.

Backbone dynamics of alamethicin bound to lipid membranes: spin-echo electron paramagnetic resonance of TOAC-spin labels

Alamethicin F50/5 is a hydrophobic peptide that is devoid of charged residues and that induces voltage-dependent ion channels in lipid membranes. The peptide backbone is likely to be involved in the ion conduction pathway. Electron spin-echo spectroscopy of alamethicin F50/5 analogs in which a selected Aib residue (at position n = 1, 8, or 16) is replaced by the TOAC amino-acid spin label was used to study torsional dynamics of the peptide backbone in association with phosphatidylcholine bilayer membranes. Rapid librational motions of limited angular amplitude were observed at each of the three TOAC sites by recording echo-detected spectra as a function of echo delay time, 2tau. Simulation of the time-resolved spectra, combined with conventional EPR measurements of the librational amplitude, shows that torsional fluctuations of the peptide backbone take place on the subnanosecond to nanosecond timescale, with little temperature dependence. Associated fluctuations in polar fields from the peptide could facilitate ion permeation.

Lateral pressure profile, spontaneous curvature frustration, and the incorporation and conformation of proteins in membranes

Lipid-protein interactions are an important determinant of the stability and function of integral and transmembrane proteins. In addition to local interactions at the lipid-protein interface, global interactions such as the distribution of internal lateral pressure may also influence protein conformation. It is shown here that the effects of the membrane lateral pressure profile on the conformation or insertion of proteins in membranes are equivalent to the elastic response to the frustrated spontaneous curvature, c(o), of the component lipid monolayer leaflets. The chemical potential of the protein in the membrane is predicted to depend linearly on the spontaneous curvature of the lipid leaflets, just as does the contribution of the protein to the elastic bending energy of the lipid, and to be independent of the hydrophobic tension, gamma(phob), at the lipid-water interface. Analysis of the dependence of protein partitioning or conformational transitions on spontaneous curvature of the constituent lipids gives an experimental estimate for the cross-sectional intramembrane shape of the protein or its difference between conformations. Values in the region of 50-110 A(2) are estimated for the effective cross-sectional shape changes on the insertion and conductance transitions of alamethicin, and on the activation of CTP:phosphocholine cytidylyltransferase or rhodopsin in lipid membranes. Much larger values are estimated for the mechanosensitive channel, MscL. Values for the change in intramembrane shape may also be used, together with determinations of lipid relative association constants, to estimate contributions of direct lipid-protein interactions to the lateral pressure experienced by the protein. Changes in chemical potential approximately 12 kJ mol(-1) can be estimated for radial changes of 1 A in a protein of diameter 40 A.

TOAC spin labels in the backbone of alamethicin: EPR studies in lipid membranes

Alamethicin is a 19-amino-acid residue hydrophobic peptide that produces voltage-dependent ion channels in membranes. Analogues of the Glu(OMe)(7,18,19) variant of alamethicin F50/5 that are rigidly spin-labeled in the peptide backbone have been synthesized by replacing residue 1, 8, or 16 with 2,2,6,6-tetramethyl-piperidine-1-oxyl-4-amino-4-carboxyl (TOAC), a helicogenic nitroxyl amino acid. Conventional electron paramagnetic resonance spectra are used to determine the insertion and orientation of the TOAC(n) alamethicins in fluid lipid bilayer membranes of dimyristoyl phosphatidylcholine. Isotropic (14)N-hyperfine couplings indicate that TOAC(8) and TOAC(16) are situated in the hydrophobic core of the membrane, whereas the TOAC(1) label resides closer to the membrane surface. Anisotropic hyperfine splittings show that alamethicin is highly ordered in the fluid membranes. Experiments with aligned membranes demonstrate that the principal diffusion axis lies close to the membrane normal, corresponding to a transmembrane orientation. Combination of data from the three spin-labeled positions yields both the dynamic order parameter of the peptide backbone and the intramolecular orientations of the TOAC groups. The latter are compared with x-ray diffraction results from alamethicin crystals. Saturation transfer electron paramagnetic resonance, which is sensitive to microsecond rotational motion, reveals that overall rotation of alamethicin is fast in fluid membranes, with effective correlation times <30 ns. Thus, alamethicin does not form large stable aggregates in fluid membranes, and ionic conductance must arise from transient or voltage-induced associations.

Orientation and lipid-peptide interactions of gramicidin A in lipid membranes: polarized attenuated total reflection infrared spectroscopy and spin-label electron spin resonance

Gramicidin A was incorporated at a peptide/lipid ratio of 1:10 mol/mol in aligned bilayers of dimyristoyl phosphatidylcholine (DMPC), phosphatidylserine (DMPS), phosphatidylglycerol (DMPG), and phosphatidylethanolamine (DMPE), from trifluoroethanol. Orientations of the peptide and lipid chains were determined by polarized attenuated total reflection infrared spectroscopy. Lipid-peptide interactions with gramicidin A in DMPC bilayers were studied with different spin-labeled lipid species by using electron spin resonance spectroscopy. In DMPC membranes, the orientation of the lipid chains is comparable to that in the absence of peptide, in both gel and fluid phases. In gel-phase DMPC, the effective tilt of the peptide exceeds that of the lipid chains, but in the fluid phase both are similar. For gramicidin A in DMPS, DMPG, and DMPE, the degree of orientation of the peptide and lipid chains is less than in DMPC. In the fluid phase of DMPS, DMPG, and DMPE, gramicidin A is also less well oriented than are the lipid chains. In DMPE especially, gramicidin A is largely disordered. In DMPC membranes, three to four lipids per monomer experience direct motional restriction on interaction with gramicidin A. This is approximately half the number of lipids expected to contact the intramembranous perimeter of the gramicidin A monomer. A selectivity for certain negatively charged lipids is found in the interaction with gramicidin A in DMPC. These results are discussed in terms of the integration of gramicidin A channels in lipid bilayers, and of the interactions of lipids with integral membrane proteins.

Infrared Dichroism of Isotope-edited α-Helices and β-Sheets

Isotope editing of amide infrared bands not only localises secondary structural elements within the protein but also yields conformational information that is not available from the linear dichroism of aligned samples without isotope editing. The additional information that can be derived on the orientational distribution of alpha-helices in membranes by the combined use of different amide bands and several positions of labelling is presented here. Also, the relationship between the azimuthal orientation of the transition moment and the protein structure is treated explicitly. A comprehensive analysis of the infrared dichroism for beta-sheets and beta-barrels is given here, for the first time. The orientation of the individual transition moments in a beta-sheet that is essential for this analysis is derived for the different amide bands.

Lipid chain length effect on the phase behaviour of PCs/PEG:2000-PEs mixtures. A spin label electron spin resonance and spectrophotometric study

Spin-label electron spin resonance (ESR) spectroscopy and spectrophotometry at fixed wavelength are used to study fully hydrated aqueous dispersions of phosphatidylcholines (PCs) with poly(ethylene glycol:2000)-phosphatidylethanolamines (PEG:2000-PEs). PEG:2000-PE is a micelle-forming polymer-lipid that is extensively used for increasing the lifetime of PC liposomes in the blood circulation through a steric stabilisation effect. The PC lipids and the PEG:2000-PE polymer-lipids have the same acyl chain length of either dimiristoyl (DM) or distearoyl (DS) chains. DMPC/PEG:2000-DMPE and DSPC/PEG:2000-DSPE mixtures were investigated over the entire range of relative compositions (0-100 mol%). In both dispersions, the low-temperature conventional spin label ESR spectra and the temperature dependence of the absorbance at 400 nm give an indication of the conversion from lamellae to micelles with increasing PEG:2000-PEs content. The physical state of the lipid assemblies, lamellar or micellar, is dependent not only on PEG:2000-PEs content, but also on the length of hydrocarbon chain of the lipid matrix. Micellisation is attained more readily in dispersions with longer hydrocarbon chains (i.e. in DSPC/PEG:2000-DSPE mixtures) than in those with shorter acyl chains (i.e. in DMPC/PEG:2000-DMPE mixtures). Saturation transfer ESR (ST-ESR) and absorbance measurements reflect the disaggregation of the bilayers and a reduction in the size of the lipid aggregates by PEG:2000-PEs at low content.

Tilt, twist, and coiling in beta-barrel membrane proteins: relation to infrared dichroism

The x-ray coordinates of beta-barrel transmembrane proteins from the porins superfamily and relatives are used to calculate the mean tilt of the beta-strands and their mean local twist and coiling angles. The 13 proteins examined correspond to beta-barrels with 8 to 22 strands, and shear numbers ranging from 8 to 24. The results are compared with predictions from the model of Murzin, Lesk, and Chothia for symmetrical regular barrels. Good agreement is found for the mean strand tilt, but the twist angles are smaller than those for open beta-sheets and beta-barrels with shorter strands. The model is reparameterised to account for the reduced twist characteristic of long-stranded transmembrane beta-barrels. This produces predictions of both twist and coiling angles that are in agreement with the mean values obtained from the x-ray structures. With the optimized parameters, the model can then be used to determine twist and coiling angles of transmembrane beta-barrels from measurements of the amide band infrared dichroism in oriented membranes. Satisfactory agreement is obtained for OmpF. The strand tilt obtained from the x-ray coordinates, or from the reparameterised model, can be combined with infrared dichroism measurements to obtain information on the orientation of the beta-barrel assembly in the membrane.

Orientation of the infrared transition moments for an alpha-helix

Appropriate values for the orientation of the amide transition dipoles are essential to the growing use of isotopically edited vibrational spectroscopy generally in structural biology and to infrared dichroism measurements on membrane-associated alpha-helices, in particular. The orientations of the transition moments for the amide vibrations of an alpha-helix have been determined from the ratio of intensities of the A- and E(1)-symmetry modes in the infrared spectra of poly(gamma-methyl-L-glutamate)(x)-co-(gamma-n-octadecyl-L-glutamate)( y) oriented on silicon substrates. Samples possessing a high degree of alignment were used to facilitate band fitting. Consistent results were obtained from both attenuated total reflection and transmission experiments with polarized radiation, yielding values of Theta(I) = 38 degrees, Theta(II) = 73 degrees, and Theta(A) = 29 degrees, relative to the helix axis, for the amide I, amide II, and amide A bands, respectively. The measurements are discussed both in the context of the somewhat divergent older determinations, and in relation to the helix geometry and results on model amide compounds, to resolve current uncertainties in the literature.

Infrared dichroism of twisted beta-sheet barrels. The structure of E. coli outer membrane proteins

The infrared dichroic ratios of the amide bands from oriented beta-barrels yield an experimental value for the mean orientation, beta, of the beta-strands, relative to the barrel axis. For a barrel of n strands, this then gives the shear number, S, that characterizes the stagger of the beta-sheet. Combining values of beta and n specifies the barrel geometry by using the optimized model of Murzin, Lesk & Chothia for regular barrels. Application to published infrared data on the Escherichia coli outer membrane protein, OmpA yields S=9-10 (n=8), a barrel radius of 0.81(+/-0.01) nm, and an internal free volume of 0.031 nm(3) per residue, where the average twist of the beta-sheets is theta approximately 28 degrees, and their coiling angle is epsilon approximately 1 degrees. Hydrophobic matching of the 2.6 nm transmembrane stretch partly determines the shear number of the OmpA beta-barrel.

Molecular and mesoscopic properties of hydrophilic polymer-grafted phospholipids mixed with phosphatidylcholine in aqueous dispersion: interaction of dipalmitoyl N-poly(ethylene glycol)phosphatidylethanolamine with dipalmitoylphosphatidylcholine studied by spectrophotometry and spin-label electron spin resonance

Spin-label electron spin resonance (ESR) spectroscopy, together with optical density measurements, has been used to investigate, at both the molecular and supramolecular levels, the interactions of N-poly(ethylene glycol)-phosphatidylethanolamines (PEG-PE) with phosphatidylcholine (PC) in aqueous dispersions. PEG-PEs are micelle-forming hydrophilic polymer-grafted lipids that are used extensively for steric stabilization of PC liposomes to increase their lifetimes in the blood circulation. All lipids had dipalmitoyl (C16:0) chains, and the polymer polar group of the PEG-PE lipids had a mean molecular mass of either 350 or 2000 Da. PC/PEG-PE mixtures were investigated over the entire range of relative compositions. Spin-label ESR was used quantitatively to investigate bilayer-micelle conversion with increasing PEG-PE content by measurements at temperatures for which the bilayer membrane component of the mixture was in the gel phase. Both saturation transfer ESR and optical density measurements were used to obtain information on the dependence of lipid aggregate size on PEG-PE content. It is found that the stable state of lipid aggregation is strongly dependent not only on PEG-PE content but also on the size of the hydrophilic polar group. These biophysical properties may be used for optimized design of sterically stabilized liposomes.

Quantitation of secondary structure in ATR infrared spectroscopy

Polarized attenuated total reflection infrared spectroscopy of aligned membranes provides essential information on the secondary structure content and orientation of the associated membrane proteins. Quantitation of the relative content of different secondary structures, however, requires allowance for geometric relations of the electric field components (E(x), E(y), E(z)) of the evanescent wave, and of the components of the infrared transition moments, in combining absorbances (A and A(perpendicular)) measured with radiation polarized parallel with and perpendicular to, respectively, the plane of incidence. This has hitherto not been done. The appropriate combination for exact evaluation of relative integrated absorbances is A + (2E(z)(2)/E(y)(2) - E(x)(2)/E(y)(2))A(perpendicular), where z is the axis of ordering that is normal to the membrane plane, and the x-axis lies in the membrane plane within the plane of incidence. This combination can take values in the range approximately from A - 0.4A(perpendicular) to A + 2.7A(perpendicular), depending on experimental conditions and the attenuated total reflection crystal used. With unpolarized radiation, this correction is not possible. Similar considerations apply to the dichroic ratios of multicomponent bands, which are also treated.

Oligomerization and structural changes of the pore-forming Pseudomonas aeruginosa cytotoxin

Pseudomonas aeruginosa produces a pathogenic factor, the 29-kDa pore-forming protein cytotoxin. Nonspecific oligomers of cytotoxin up to the hexamer, induced by oxidative crosslinking or detergent micellae, were based on intermolecular disulfide bridges. SDS induced tetramer, hexamer and mainly pentamers that were resistant to reducing conditions, indicating an additional oligomerization mechanism. Functional oligomerization after incubation with different membranes resulted in an oligomer of approximately 145 kDa that was identified as the pentamer by comparison with the SDS-induced oligomers. Covalent modification with diethylpyrocarbonate showed that histidine residues are indispensable for functional pentamerization. Pentamer formation was not influenced by the lipid composition of the liposomes tested, indicating that rising membrane fluidity did not increase oligomerization. The secondary structure of cytotoxin determined by spectroscopy is characterized by approximately 50% beta-sheet, 20% beta-turn, 10% alpha-helix and 20% remaining structure. Contact with detergent micellae or liposomes induced a reorganization of beta-structure associations, as observed by attenuated total reflection-Fourier transform infrared spectroscopy. Electron microscopy and principle component analysis of the cytotoxin monomer demonstrated a tapered molecule of 11 nm in length and a maximum width of 3.5 nm. These results classify the cytotoxin as a pore-forming toxin, rich in antiparallel beta-structure, that needs to oligomerize and inserts into membranes; it is very similar to the Staphylococcus aureus alpha-toxin.