Self-association of model transmembrane alpha-helices is modulated by lipid structure

We have developed a fluorescence quenching method using peptides containing 3,5-dibromotryrosine to measure oligomerization of model transmembrane alpha-helices in lipid bilayers. Peptides of the type Ac-LysLysGlyLeu(m)XLeu(n)LysLysAla-amide where X is tryptophan or 3,5-dibromotyrosine were found to form heterodimers in bilayers of phosphatidylcholine in the liquid-crystalline phase. The free energy of dimer formation changed little with increasing number of Leu residues from 16 to 22 but increased with increasing phospholipid fatty acyl chain length, with a slope of about 0.5 kJ mol(-1) per fatty acyl chain carbon. Peptides were excluded from lipid in the gel phase, resulting in increased levels of oligomerization. Addition of cholesterol to form the liquid-ordered state led to increased dimerization but without phase separation. The presence of phosphatidylethanolamine had little effect on dimerization.     

Control of the transmembrane orientation and interhelical interactions within membranes by hydrophobic helix length

We examined the effect of the length of the hydrophobic core of Lys-flanked poly(Leu) peptides on their behavior when inserted into model membranes. Peptide structure and membrane location were assessed by the fluorescence emission lambdamax of a Trp residue in the center of the peptide sequence, the quenching of Trp fluorescence by nitroxide-labeled lipids (parallax analysis), and circular dichroism. Peptides in which the hydrophobic core varied in length from 11 to 23 residues were found to be largely alpha-helical when inserted into the bilayer. In dioleoylphosphatidylcholine (diC18:1PC) bilayers, a peptide with a 19-residue hydrophobic core exhibited highly blue-shifted fluorescence, an indication of Trp location in a nonpolar environment, and quenching localized the Trp to the bilayer center, an indication of transmembrane structure. A peptide with an 11-residue hydrophobic core exhibited emission that was red-shifted, suggesting a more polar Trp environment, and quenching showed the Trp was significantly displaced from the bilayer center, indicating that this peptide formed a nontransmembranous structure. A peptide with a 23-residue hydrophobic core gave somewhat red-shifted fluorescence, but quenching demonstrated the Trp was still close to the bilayer center, consistent with a transmembrane structure. Analogous behavior was observed when the behavior of individual peptides was examined in model membranes with various bilayer widths. Other experiments demonstrated that in diC18:1PC bilayers the dilution of the membrane concentration of the peptide with a 23-residue hydrophobic core resulted in a blue shift of fluorescence, suggesting the red-shifted fluorescence at higher peptide concentrations was due to helix oligomerization. The intermolecular self-quenching of rhodamine observed when the peptide was rhodamine-labeled, and the concentration dependence of self-quenching, supported this conclusion. These studies indicate that the mismatch between helix length and bilayer width can control membrane location, orientation, and helix-helix interactions, and thus may mismatch control both membrane protein folding and the interactions between membrane proteins.     

Cumulative effects of amino acid substitutions and hydrophobic mismatch upon the transmembrane stability and conformation of hydrophobic alpha-helices

The effects of amino acid substitutions upon the behavior of poly(Leu)-rich alpha-helices inserted into model membrane vesicles were investigated. One or two consecutive Leu residues in the hydrophobic core of the helix were substituted with A, F, G, S, D, K, H, P, GG, SS, PG, PP, KK, or DD residues. A Trp placed at the center of the sequence allowed assessment of peptide behavior via fluorescence emission lambda(max) and dual quenching analysis of Trp depth [Caputo, G. A., and London, E. (2003) Biochemistry 42, 3265-3274]. In vesicles composed of dioleoylphosphatidylcholine (DOPC), all of the peptides with single substitutions adopted a transmembrane (TM) state. Experiments were also performed in thicker bilayers composed of dierucoylphosphatidylcholine (DEuPC). In DEuPC vesicles TM states were destabilized by mismatch between helix length and bilayer thickness. Nevertheless, in DEuPC vesicles TM states were still prevalent for peptides with single substitutions, although less so for peptides with P, K, H, or D substitutions. In contrast to single substitutions, certain consecutive double substitutions strongly interfered with formation of TM states. In both DOPC and DEuPC vesicles DD and KK substitutions abolished the normal TM state, but GG and SS substitutions had little effect. In even wider bilayers, a SS substitution reduced the formation of a TM state. A peptide with a PP substitution maintained the TM state in DOPC vesicles, but in DEuPC vesicles the level of formation of the TM state was significantly reduced. Upon disruption of normal TM insertion peptides moved close to the bilayer surface, with the exception of the KK-substituted peptide in DOPC vesicles, which formed a truncated TM segment. These studies begin to provide a detailed relationship between sequence and the stability of TM insertion and show that the influence of insertion-destabilizing residues upon hydrophobic helices can be strongly modulated by properties such as mismatch. For certain helix-forming hydrophobic sequences, sensitivity to lipid structure may be sufficient to induce large conformational changes in vivo.     

Measurement of thermodynamic parameters for hydrophobic mismatch 1: self-association of a transmembrane helix

Membrane partitioning and self-association of transmembrane helices are crucial thermodynamic steps for membrane protein folding, although experimental difficulties have hampered quantitative estimations of related thermodynamic parameters, especially in lipid bilayer environments. This article reports for the first time, the complete set of thermodynamic parameters (DeltaG, DeltaH, DeltaS, and DeltaC(p)) for the formation of the antiparallel dimer of the inert hydrophobic model transmembrane helix X-(AALALAA)(3)-Y (X = 7-nitro-2-1, 3-benzoxadiazol-4-yl (NBD) and Y = NH(2) (I) or X = Ac and Y = NHCH(2)CH(2)-S-N-[4-[[4-(dimethylamino)phenyl]azo]phenyl]maleimide (DABMI) (II)) in dimonounsaturated phosphocholine lipid bilayers with different hydrophobic thicknesses (C14-C22) at 5-55 degrees C, as evaluated by fluorescence resonance energy transfer from I to II. Stronger dimerization was observed in thicker membranes and at lower temperatures (DeltaG = -9 to -26 kJ mol(-)(1)), driven by large negative DeltaH values (-18 to -80 kJ mol(-)(1)). Fourier transform infrared-polarized spectroscopy revealed that the peptide formed a stable transmembrane helix with an orientation angle of approximately 15 degrees in all bilayers without significant effects on lipid structures, suggesting that the depth to which the helix termini penetrate changes depending on the degree of hydrophobic mismatch. The enthalpy changes for helix-helix interactions can be well explained by the electrostatic interactions between helix macrodipoles in different dielectric environments. The new concept of dipole-dipole interaction as a basic driving force of helix dimerization will become a basis for understanding the structural and functional modifications in response to hydrophobic mismatch.     

Measurement of thermodynamic parameters for hydrophobic mismatch 2: intermembrane transfer of a transmembrane helix

Hydrophobic matching between proteins and lipids is essential for the thermodynamic stability of integral membrane proteins. However, there is no direct thermodynamic information available about the intermembrane transfer of proteins between membranes with different hydrophobic thicknesses, which is crucial for understanding hydrophobic mismatch. This article reports the complete set of thermodynamic parameters (DeltaG, DeltaH, DeltaS, and DeltaC(p)) for the intermembrane transfer of the inert hydrophobic model transmembrane helix NBD-(AALALAA)(3)-NH(2) (NBD: 7-nitro-2-1,3-benzoxadiazol-4-yl), which is exchangeable between vesicles, from 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) to dimonounsaturated-phosphocholine lipid bilayers with different hydrophobic thicknesses (C14-C22) at 37-58 degrees C. The transfer free energies were calculated from equilibrium values of the extent of helix transfer from donor to acceptor lipid vesicles, as monitored by a decrease in fluorescence resonance energy transfer from the NBD group to a lipid-labeled Rhodamine in the donor upon transfer to the quencher-free acceptor. Under hydrophobic mismatch conditions up to approximately 7 A, the helix partitioning became unfavorable up to +7 kJ mol(-)(1), hampered by an increase in entropic (up to +20 kJ mol(-)(1)) and enthalpic (up to +66 kJ mol(-)(1)) terms in thinner and thicker membranes, respectively. Together with the results that H/D exchange at the membrane interface was accelerated in thinner membranes the obtained thermodynamic parameters were reasonably explained assuming that hydrophobic mismatch induces aqueous exposure or membrane burial of the helix termini, resulting in excess energies originating from the hydration of terminal hydrophobic residues or the unfavorable Born energy of terminal partial charges of the helix macrodipole.     

A molecular model for lipid-protein interaction in membranes: the role of hydrophobic mismatch.

The interaction free energy between a hydrophobic, transmembrane, protein and the surrounding lipid environment is calculated based on a microscopic model for lipid organization. The protein is treated as a rigid hydrophobic solute of thickness dP, embedded in a lipid bilayer of unperturbed thickness doL. The lipid chains in the immediate vicinity of the protein are assumed to adjust their length to that of the protein (e.g., they are stretched when dP > doL) in order to bridge over the lipid-protein hydrophobic mismatch (dP-doL). The bilayer's hydrophobic thickness is assumed to decay exponentially to its asymptotic, unperturbed, value. The lipid deformation free energy is represented as a sum of chain (hydrophobic core) and interfacial (head-group region) contributions. The chain contribution is calculated using a detailed molecular theory of chain packing statistics, which allows the calculation of conformational properties and thermodynamic functions (in a mean-field approximation) of the lipid tails. The tails are treated as single chain amphiphiles, modeled using the rotational isometric state scheme. The interfacial free energy is represented by a phenomenological expression, accounting for the opposing effects of head-group repulsions and hydrocarbon-water surface tension. The lipid deformation free energy delta F is calculated as a function of dP-doL. Most calculations are for C14 amphiphiles which, in the absence of a protein, pack at an average area per head-group ao approximately equal to 32 A2 (doL approximately 24.5 A), corresponding to the fluid state of the membrane. When dP = doL, delta F > 0 and is due entirely to the loss of conformational entropy experienced by the chains around the protein. When dP > doL, the interaction free energy is further increased due to the enhanced stretching of the tails. When dP < doL, chain flexibility (entropy) increases, but this contribution to delta F is overcounted by the increase in the interfacial free energy. Thus, delta F obtains a minimum at dP-doL approximately 0. These qualitative interpretations are supported by detailed numerical calculations of the various contributions to the interaction free energy, and of chain conformational properties. The range of the perturbation of lipid order extends typically over few molecular diameters. A rather detailed comparison of our approach to other models is provided in the discussion.     

Topological stability and self-association of a completely hydrophobic model transmembrane helix in lipid bilayers

Investigation of interactions between hydrophobic model peptides and lipid bilayers is perhaps the only way to elucidate the principles of the folding and stability of membrane proteins (White, S. H., and Wimley, W. C. (1998) Biochim. Biophys. Acta 1367, 339-352). We designed the completely hydrophobic "inert" peptide modeling a transmembrane (TM) helix without any of the specific side-chain interactions expected, X-(LALAAAA)(3)-NH(2) [X = Ac (I), 7-nitro-2-1,3-benzoxadiazol-4-yl (II), or 5(6)-carboxytetramethylrhodamine (III)]. Fourier transform infrared-polarized attenuated total reflection measurements revealed that I as well as II assume a TM helix in hydrated 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine bilayers. Dithionite quenching experiments detected no topological change (flip-flop) in the helix II for at least 24 h. Thus, the TM helix itself is a highly stable structure, even in the absence of flanking hydrophilic or aromatic amino acids which are suggested to play important roles in stable TM positioning. Helix self-association in lipid bilayers was detected by fluorescence resonance energy transfer between II and III. The peptide was in a monomer-antiparallel dimer equilibrium with an association free energy of approximately -13 kJ/mol. Electron spin resonance spectra of 1-palmitoyl-2-stearoyl-(14-doxyl)-sn-glycero-3-phosphocholine demonstrated the presence of a motionally restricted component at lower temperatures.     

Prediction of transmembrane helix orientation in polytopic membrane proteins

Background  

Membrane proteins compose up to 30% of coding sequences within genomes. However, their structure determination is lagging behind compared with soluble proteins due to the experimental difficulties. Therefore, it is important to develop reliable computational methods to predict structures of membrane proteins.     

The determinants of hydrophobic mismatch response for transmembrane helices

Hydrophobic mismatch arises from a difference in the hydrophobic thickness of a lipid membrane and a transmembrane protein segment, and is thought to play an important role in the folding, stability and function of membrane proteins. We have investigated the possible adaptations that lipid bilayers and transmembrane α-helices undergo in response to mismatch, using fully-atomistic molecular dynamics simulations totaling 1.4 μs. We have created 25 different tryptophan-alanine-leucine transmembrane α-helical peptide systems, each composed of a hydrophobic alanine–leucine stretch, flanked by 1–4 tryptophan side chains, as well as the β-helical peptide dimer, gramicidin A. Membrane responses to mismatch include changes in local bilayer thickness and lipid order, varying systematically with peptide length. Adding more flanking tryptophan side chains led to an increase in bilayer thinning for negatively mismatched peptides, though it was also associated with a spreading of the bilayer interface. Peptide tilting, bending and stretching were systematic, with tilting dominating the responses, with values of up to ~ 45° for the most positively mismatched peptides. Peptide responses were modulated by the number of tryptophan side chains due to their anchoring roles and distributions around the helices. Potential of mean force calculations for local membrane thickness changes, helix tilting, bending and stretching revealed that membrane deformation is the least energetically costly of all mismatch responses, except for positively mismatched peptides where helix tilting also contributes substantially. This comparison of energetic driving forces of mismatch responses allows for deeper insight into protein stability and conformational changes in lipid membranes.     

The net orientation of nicotinic receptor transmembrane alpha-helices in the resting and desensitized states

The net orientation of nicotinic acetylcholine receptor transmembrane alpha-helices has been probed in both the activatable resting and nonactivatable desensitized states using linear dichroism Fourier-transform infrared spectroscopy. Infrared spectra recorded from reconstituted nicotinic acetylcholine receptor membranes after 72 h exposure to (2)H2O exhibit an intense amide I component band near 1655 cm(-1) that is due predominantly to hydrogen-exchange-resistant transmembrane peptides in an alpha-helical conformation. The measured dichroism of this band is 2.37, suggesting a net tilt of the transmembrane alpha-helices of roughly 40 degrees from the bilayer normal, although this value overestimates the tilt angle because the measured dichroism at 1655 cm(-1) also reflects the dichroism of overlapping amide I component bands. Significantly, no change in the net orientation of the transmembrane alpha-helices is observed upon agonist binding. In fact, the main changes in structure and orientation detected upon desensitization involve highly solvent accessible regions of the polypeptide backbone. Our data are consistent with a capping of the ligand binding site by the solvent accessible C-loop with little change in the structure of the transmembrane domain in the desensitized state. Changes in structure at the interface between the ligand-binding and transmembrane domains may uncouple binding from gating.     

Structural role of glycine in amyloid fibrils formed from transmembrane alpha-helices

Amyloid fibrils associated with diseases such as Alzheimer's are often derived from the transmembrane helices of membrane proteins. It is known that the fibrils have a cross-beta-sheet structure where main chain hydrogen bonding occurs between beta-strands in the direction of the fibril axis. However, the structural basis for how the membrane-spanning helix is converted into a beta-sheet or how protofibrils associate into fibrils is not known. Here, we use a model peptide corresponding to a portion of the single transmembrane helix of glycophorin A to investigate the structural role of glycine in amyloid-like fibrils formed from transmembrane helices. Glycophorin A contains a GxxxG motif that is found in many transmembrane sequences including that of the amyloid precursor protein and prion protein. We propose that glycine, which mediates helix interactions in membrane proteins, also provides key packing motifs when it occurs in beta-sheets. We show that glycines in the glycophorin A transmembrane helix promote extended beta-strand formation when the helix partitions into aqueous environments and stabilize the packing of beta-sheets in the formation of amyloid-like fibrils. We demonstrate that fibrillization can be disrupted with a new class of inhibitors that target the molecular grooves created by glycine.     

Tilt angle of a trans-membrane helix is determined by hydrophobic mismatch

In order to investigate the compensation mechanism of a trans-membrane helix in response to hydrophobic mismatch, the tilt and rotation angles of the trans-membrane helix of Vpu aligned in lipid bilayers of various thickness were determined using orientation-dependent frequencies obtained from solid-state NMR experiments of aligned samples. A tilt angle of 18 degrees was observed in 18:1-O-PC/DOPG (9:1) lipid bilayers, which have a hydrophobic thickness that approximately matches the hydrophobic length of the trans-membrane helix of Vpu. Upon decreasing the hydrophobic thickness of lipid bilayers, no significant change in rotation angle was observed. However, the tilt angle increased systematically with increasing positive mismatch to 27 degrees in 14:0-O-PC/DMPG (9:1), 35 degrees in 12:0-O-PC/DLPG (9:1), and 51 degrees in 10:0 PC/10:0 PG (9:1) lipid bilayers, indicating that the change in tilt angle of the trans-membrane helix is a principal compensation mechanism for hydrophobic mismatch. In addition, the distinctive kink in the middle of the helix observed in 18:1 bilayers disappears in thinner bilayers. Although the opposite of what might be expected, this finding suggests that a helix kink may also be a part of the hydrophobic matching mechanism for trans-membrane helices.     

Asparagine-mediated self-association of a model transmembrane helix

In membrane proteins, the extent to which polarity, hydrogen bonding, and van der Waals packing interactions of the buried, internal residues direct protein folding and association of transmembrane segments is poorly understood. The energetics associated with these various interactions should differ substantially between membrane versus water-soluble proteins. To help evaluate these energetics, we have altered a water-soluble, two-stranded coiled-coil peptide to render its sequence soluble in membranes. The membrane-soluble peptide associates in a monomer-dimer-trimer equilibrium, in which the trimer predominates at the highest peptide/detergent ratios. The oligomers are stabilized by a buried Asn side chain. Mutation of this Asn to Val essentially eliminates oligomerization of the membrane-soluble peptide. Thus, within a membrane-like environment, interactions involving a polar Asn side chain provide a strong thermodynamic driving force for membrane helix association.     

Effects of aromatic residues at the ends of transmembrane alpha-helices on helix interactions with lipid bilayers

We have studied the effects of aromatic residues at the ends of peptides of the type Ac-KKGL(n)()WL(m)()KKA-amide on their interactions with lipid bilayers as a function of lipid fatty acyl chain length, physical phase, and charge. Peptide Ac-KKGFL(6)WL(8)FKKA-amide (F(2)L(14)) incorporated into bilayers of phosphatidylcholines containing monounsaturated fatty acyl chains of lengths C14-C24 at a peptide:lipid molar ratio of 1:100 in contrast to Ac-KKGL(7)WL(9)KKA-amide (L(16)) which did not incorporate at all into dierucoylphosphatidylcholine [di(C24:1)PC]; Ac-KKGYL(6)WL(8)YKKA-amide (Y(2)L(14)) incorporated partly into di(C24:1)PC. Lipid-binding constants relative to that for dioleoylphosphatidylcholine (C18:1)PC were obtained using a fluorescence quenching method. For Y(2)L(14) and F(2)L(14), relative lipid-binding constants increased with increasing fatty acyl chain length from C14 to C24; strongest binding did not occur at the point where the hydrophobic length of the peptide equalled the hydrophobic thickness of the bilayer. For Ac-KKGYL(9)WL(11)YKKA-amide (Y(2)L(20)), increasing chain length from C18 to C24 had little effect on relative binding constants. Anionic phospholipids bound more strongly than zwitterionic phospholipids to Y(2)L(14) and Y(2)L(20) but effects of charge were relatively small. In two phase (gel and liquid crystalline) mixtures, all the peptides partitioned more strongly into liquid crystalline than gel phase; effects were independent of the structure of the peptide or of the lipid (dipalmitoylphosphatidylcholine or bovine brain sphingomyelin). Addition of cholesterol had little effect on incorporation of the peptides into lipid bilayers. It is concluded that the presence of aromatic residues at the ends of transmembrane alpha-helices effectively buffers them against changes in bilayer thickness caused either by an increase in the chain length of the phospholipid or by the presence of cholesterol.     

Peptide antibiotic trichogin in model membranes: Self-association and capture of fatty acids

The antimicrobial action of peptides in bacterial membranes is commonly related to their mode of self-assembling which results in pore formation. To optimize peptide antibiotic use for therapeutic purposes, a study on the concentration dependence of self-assembling process is thus desirable. In this work, we investigate this dependence for peptaibol trichogin GA IV (Tric) in the 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) model membrane in the range of peptide concentrations between 0.5 and 3.3?mol%. Pulsed double electron-electron resonance (PELDOR) applied on spin-labeled peptide analogs highlights the onset of peptide dimerization above a critical peptide concentration value, namely ~ 2?mol%. Electron spin echo (ESE) envelope modulation (ESEEM) for D₂O-hydrated bilayers shows that dimerization is accompanied by peptide re-orientation towards a trans-membrane disposition. For spin-labeled stearic acids (5-DSA) in POPC bilayers, the study of ESE decays and ESEEM in the presence of a deuterated peptide analog indicates that above the critical peptide concentration the 5-DSA molecules are attracted by peptide molecules, forming nanoclusters. As the 5-DSA molecules represent a model for the behavior of fatty acids participating in bacterial membrane homeostasis, such capturing action by Tric may represent an additional mechanism of its antibiotic activity.     

Effect of hydrophobic mismatch on phase behavior of lipid membranes

We investigate the competing effects of hydrophobic mismatch and chain stretching on the morphology and evolution of domains in lipid membranes via Monte Carlo techniques. We model the membrane as a binary mixture of particles that differ in their preferred lengths, with the shorter particles mimicking unsaturated nonraft lipids and the longer particles mimicking saturated raft lipids. We find that phase separation can be induced upon increasing either the ratio J/kappa of the hydrophobic surface tension J to the compressibility modulus kappa. J/kappa determines the decay length for thickness changes. When this decay length is larger than the system size the membrane remains mixed. Furthermore, increasing the thickness relaxation time can induce transient phase separation.     

The control of transmembrane helix transverse position in membranes by hydrophilic residues

The ability of hydrophilic residues to shift the transverse position of transmembrane (TM) helices within bilayers was studied in model membrane vesicles. Transverse shifts were detected by fluorescence measurements of the membrane depth of a Trp residue at the center of a hydrophobic sequence. They were also estimated from the effective length of the TM-spanning sequence, derived from the stability of the TM configuration under conditions of negative hydrophobic mismatch. Hydrophilic residues (at the fifth position in a 21-residue hydrophobic sequence composed of alternating Leu and Ala residues and flanked on both ends by two Lys) induced transverse shifts that moved the hydrophilic residue closer to the membrane surface. At pH 7, the dependence of the extent of shift upon the identity of the hydrophilic residue increased in the order: L < GYT < RH < S < P < K < EQ < N < D. By varying pH, shifts with ionizable residues fully charged or uncharged were measured, and the extent of shift increased in the order: L < GYH^oT < E^oR < S < P < K⁺< QD^oH⁺ < NE^– < D^–. The dependence of transverse shifts upon hydrophilic residue identity was consistent with the hypothesis that shift magnitude is largely controlled by the combination of side chain hydrophilicity, ionization state, and ability to position polar groups near the bilayer surface (snorkeling). Additional experiments showed that shift was also modulated by the position of the hydrophilic residue in the sequence and the hydrophobicity of the sequence moved out of the bilayer core upon shifting. Combined, these studies show that the insertion boundaries of TM helices are very sensitive to sequence, and can be altered even by weakly hydrophilic residues. Thus, many TM helices may have the capacity to exist in more than one transverse position. Knowledge of the magnitudes of transverse shifts induced by different hydrophilic residues should be useful for design of mutagenesis studies measuring the effect of transverse TM helix position upon function.     

FTIR spectroscopic studies of the conformation and amide hydrogen exchange of a peptide model of the hydrophobic transmembrane alpha-helices of membrane proteins.

The conformation and amide hydrogen exchangeability of the hydrophobic peptide Lys2-Gly-Leu24-Lys2-Ala-amide were studied by Fourier transform infrared spectroscopy. In these studies information on the secondary structure of the peptide was obtained from an examination of the contours of both the amide I and amide II absorption bands. The conformationally sensitive amide I and amide II regions of the infrared spectra suggest that the peptide is predominantly alpha-helical and that it contains some non-alpha-helical structures which are probably in an extended conformation. Studies of the exchangeability of the amide protons of the peptide indicate that there are two populations of amide protons which differ markedly with respect to their exchangeability with the bulk solvent phase, whether the peptide is dissolved in methanol or dispersed in hydrated lipid bilayers. One population of amide protons is very readily exchangeable, and our data suggest that it arises primarily but not exclusively from the extended regions of the peptide. The other population exchanges very slowly with the bulk solvent and appears to originate entirely from the alpha-helical domain of the peptide. This latter population is virtually unexchangeable when the peptide is dispersed in hydrated phosphatidylcholine bilayers but can be largely exchanged when the peptide is solubilized with methanol. We suggest that this slowly exchanging population of amide protons arises from the central part of the hydrophobic polyleucine core which forms a very stable alpha-helix that would be deeply buried in the hydrophobic domain of hydrated lipid bilayers.(ABSTRACT TRUNCATED AT 250 WORDS)