Conformational studies of human [15-2-aminohexanoic acid]little gastrin in sodium dodecyl sulfate micelles by 1H NMR

Human little gastrin is a 17 amino acid peptide that adopts a random conformation in water and an ordered structure in sodium dodecyl sulfate (SDS) micelles as well as in trifluoroethanol (TFE). The circular dichroism spectra in these two media have the same shape, indicative of a similar preferred conformation [Mammi, S., Mammi, N. J., Foffani, M. T., Peggion, E., Moroder, L., & Wünsch, E. (1987) Biopolymers 26, S1-S10]. We describe here the assignment of the proton NMR resonances and the conformational analysis of [Ahx15]little gastrin in SDS micelles. Two-dimensional correlation techniques form the basis for the assignment. The conformational analysis utilized NOE's, NH to C alpha H coupling constants, and the temperature coefficients of the amide chemical shifts. The NMR data indicate a helical structure in the N-terminal portion of the peptide. These results are compared with the conformation that we recently proposed for a minigastrin analogue (fragment 5-17 of [Ahx15]little gastrin) in TFE.     

Kinetics of amide proton exchange in helical peptides of varying chain lengths. Interpretation by the Lifson-Roig equation.

The kinetics of amide proton exchange (1H----2H) have been measured by proton nuclear magnetic resonance spectroscopy for a set of helical peptides with the generic formula Ac-(AAKAA)m Y-NH2 and with chain lengths varying from 6 to 51 residues. The integrated intensity of the amide resonances has been measured as a function of time in 2H2O at pH* 2.50. Exchange kinetics for these peptides can be modeled by applying the Lifson-Roig treatment for the helix-to-coil transition. The Lifson-Roig equation is used to compute the probability that each residue is helical, as defined by its backbone (phi, psi) angles. A recursion formula then is used to find the probability that the backbone amide proton of each residue is hydrogen bonded. The peptide helix can be treated as a homopolymer, and direct exchange from the helix can be neglected. The expression for the exchange kinetics contains only three unknown parameters: the rate constant for exchange of a non-hydrogen-bonded (random coil) backbone amide proton and the nucleation (v2) and propagation (w) parameters of the Lifson-Roig theory. The fit of the exchange curves to these three parameters is very good, and the values for v2 and w agree with those derived from circular dichroism studies of the thermally-induced unfolding of related peptides [Scholtz, J.M., Qian, H., York, E.J., Stewart, J.M., & Baldwin, R.L. (1991) Biopolymers (in press]).     

1H-NMR conformational analysis of a high-affinity antigenic 11-residue peptide from the tryptophan synthase beta 2 subunit.

Two synthetic peptides from the beta 2 subunit of tryptophan synthase have been studied by 1H-NMR spectroscopy at 300 MHz. One peptide, His-Gly-Arg-Val-Gly-Ile-Tyr-Phe-Gly-Met-Lys (peptide 11; Ile, isoleucine) is antigenic and binds with a high affinity to a monoclonal antibody that recognizes the native beta 2 subunit. The second peptide, His-Gly-Arg-Val-Gly-Ile-Tyr-Phe (peptide 8) reacts very weakly with the antibody. The 1H-NMR spectra of the two peptides have been assigned from two-dimensional techniques in H2O, 2H2O and (2H6) dimethyl sulfoxide [(2H6)Me2SO]. The structure has been evaluated through analysis of nuclear Overhauser effects, coupling constants, amide-proton exchange rates and their temperature coefficients, and chemical shifts. In aqueous solvent, the C-terminal part of peptide 11 presents some structure centered around residues Phe-Gly-Met. The relationship between the structure found in peptide 11 and its antigenic nature is discussed.     

Conformation of the glycotripeptide repeating unit of antifreeze glycoprotein of polar fish as determined from the fully assigned proton n.m.r. spectrum

With its simple glycotripeptide repeating structure the antifreeze glycoprotein of polar fish may be an especially simple conformational mode for mucin glycoproteins with similar but more complex structures. The fully assigned proton n.m.r. spectrum confirms the anomeric configurations of the hexapyranosidic sugars of the side chains and the coupling constants of the alpha GalNAc and the beta Gal residues show both to be in the expected 4C1 chair conformation. The assignment of a single resonance for each proton of the (Ala-Thr-Ala)n repeat unit coupled with the observation of long range nuclear Overhauser effects (n.O.e.) implies a three-fold repeating conformation. The resonances of the two alanines are distinct and can be assigned to their correct positions in the peptide sequence by n.O.e. observed at the amide proton resonances on saturation of the alpha proton signals. The amide proton coupling constants of all three peptide residues are similar and imply a limited range of peptide backbone torsion angles, phi CN. The large n.O.e. which has been observed between the amide proton and the alpha proton of the residue preceding it in the sequence implies large positive values for the peptide dihedral angle, psi CC. Limits are placed on possible values of side chain dihedral angles by the observation of the coupling constant between the alpha and beta protons of the threonyl residue. The observation of n.O.e. between the anomeric proton of GalNAc and the threonyl side chain protons gives information on the conformation of the alpha glycosidic linkage between the disaccharide and the peptide. n.O.e. observed between the protons of the beta glycosidic linkage indicates the conformation of the disaccharide and the large amide proton coupling constant of the GalNAc residue shows a trans proton relationship. The spectroscopically derived data have been combined with conformational energy calculations to give a conformational model for antifreeze glycoprotein in which the hydrophobic surfaces of the disaccharide side chains are wrapped closely against a three-fold left handed helical peptide backbone. The hydrophilic sides of the disaccharides are aligned so that they may bind to the ice crystal face, which is perpendicular to the fast growth axis inhibiting normal crystal growth.     

A study of the structure of human complement component factor H by Fourier transform infrared spectroscopy and secondary structure averaging methods

Fourier transform infrared spectroscopy was used to investigate the secondary structure of human complement component factor H in H2O and 2H2O buffers. The spectra show a broad amide I band which after second-derivative calculations is shown to be composed of three components at 1645, 1663, and 1685 cm-1 in H2O and at 1638, 1661, and 1680 cm-1 in 2H2O. The frequencies of these components are consistent with the existence of an extensive antiparallel beta-strand secondary structure. The exchange properties of the amide protons of factor H as measured in 2H2O buffers are rapid and lead to an estimate of NH proton nonexchange that is comparable with those for small globular proteins. Human factor H is constructed from a linear sequence of 20 short consensus repeats with a mean of 61 residues in each one. To investigate the secondary structure further, secondary structure predictions were carried out on the basis of an alignment scheme for 101 sequences for these repeats as found in human factor H and 12 other proteins. These predictions were averaged in order to improve the reliability of the calculations. Both the Robson and the Chou-Fasman methods indicate significant beta-structural contents. Residues 21-51 in the 61-residue repeat show a clear prediction of four strands of beta-structure and four beta-turns. A structural model based on antiparallel beta-strands in the secondary structure is proposed and discussed.(ABSTRACT TRUNCATED AT 250 WORDS)     

1H and 15N NMR characterization of free and bound states of an amphiphilic peptide interacting with calmodulin.

A peptide of 17 amino acid residues Ac-L-K-W-K-K-L-L-K-L-L-K-K-L-L-K-L-G-NH2, designed to form an amphiphilic basic alpha-helix [DeGrado, W.F., Prendergast, F. G., Wolfe, H. R., Jr., & Cox, J. A. (1985) J. Cell. Biochem. 29, 83-93], was labeled with 15N at positions 1, 7, 9, and 10. Homo- and heteronuclear NMR techniques were used to characterize the conformational changes of the peptide when it binds to calmodulin in the presence of Ca2+ ions. The spectrum of the free peptide in aqueous solution at pH 6.3 and 298 K was completely assigned by a combined application of several two-dimensional proton NMR methods. Analysis of the short- and medium-range NOE connectivities and of the secondary chemical shifts indicated that the peptide populates, to a significant extent, an alpha-helix conformational state, in agreement with circular dichroism measurements under similar physicochemical conditions. 15N-edited 1D spectra and 15N(omega 2)-half-filtered two-dimensional NMR experiments on the peptide in a 1:1 complex with calmodulin allowed assignment of half of the amide proton resonances and three C alpha H resonances of the bound peptide. The observed NOE connectivities between the peptide backbone protons are indicative of a stable helical secondary structure spanning at least the fragment L1-K11. The equilibrium and dynamic NMR parameters of the bound peptide are discussed in terms of a molecular interaction model.     

CD and NMR investigations on trifluoroethanol-induced step-wise folding of helical segment from scorpion neurotoxin.

A 14 amino acid residue peptide from the helical region of Scorpion neurotoxin has been structurally characterized using CD and NMR spectroscopy in different solvent conditions. 2,2,2-Trifluoroethanol (TFE) titration has been carried out in 11 steps from 0 to 90% TFE and the gradual stabilization of the conformation to form predominantly alpha-helix covering all of the 14 residues has been studied by 1H and 13C NMR spectroscopy. Detailed information such as coupling constants, chemical shift indices, NOESY peak intensities and amide proton temperature coefficients at each TFE concentration has been extracted and analysed to derive the step-wise preferential stabilization of the helical segments along the length of the peptide. It was found that there is a finite amount of the helical conformation in the middle residues 5-11 even at low TFE concentrations. It was also observed that > 75% TFE (v/v) is required for the propagation of the helix to the N and C termini and for correct packing of the side chains of all of the residues. These observations are significant to understanding the folding of this segment in the protein and may throw light on the inherent preferences and side chain interactions in the formation of the helix in the peptide.     

Secondary structure of a herpes simplex virus glycoprotein D antigenic domain

The peptide 6-amino caproyl-Pro-Ser-Leu-Lys-Met-Ala-Asp-Pro-Asn-Arg-Phe-Arg-Gly-Lys-Asp-Leu- Pro-6- amino caproate has been synthesized and its secondary structure has been investigated by 1H n.m.r. at 400 MHz. Resonances were assigned from 2D NOESY and COSY spectra, and the secondary structure was determined using NOEs, three-bond coupling constants, and exchange rates of amide protons. The peptide has two tight turns centered on the Pro-Asn and Arg-Gly pairs. The relationship between the secondary structure found here and the antigenic nature of the peptide is discussed.     

1H NMR resonance assignments, secondary structure, and global fold of Apo bovine calbindin D9k

The solution structure and dynamics of apo bovine calbindin D9k have been studied by a wide range of two-dimensional 1H nuclear magnetic resonance experiments. Due to the presence of conformational heterogeneity in the wild-type protein, the sequential resonance assignment was carried out on a Pro43----Gly mutant. By use of a combination of scalar correlation experiments acquired from H2O solution, 61 of the 76 1H spin systems could be assigned to particular amino acid types. The remaining resonances were assigned by a parallel series of experiments acquired from 2H2O solution. These spin system assignments provided a basis for complete sequential resonance assignments from interresidue backbone nuclear Overhauser effects (NOEs). Elements of secondary structure were identified from sequential and medium-range NOEs, backbone spin-spin coupling constants, and slowly exchanging amide protons. Four sections of helix are delineated, together with a short antiparallel beta-sheet interaction between the peptide loops involved in Ca2+ binding. The global fold is provided by combining these elements of secondary structure with a subset of the long-range, interhelix NOEs. Comparison with similar studies on the Ca2(+)-saturated protein indicates that at this crude level the structures are very similar. However, removal of the Ca2+ does dramatically affect the dynamics of the protein, as judged by amide proton exchange rates and aromatic ring rotation. This is particularly evident in the increased flexibility of the residues in the hydrophobic core.     

Beware of proteins in DMSO

The effect on the secondary structure of representative alpha-helical, beta-sheet and disordered proteins by varying concentrations of dimethyl sulphoxide (DMSO) in 2H2O has been investigated by Fourier transform infrared spectroscopy. Significant perturbations of protein secondary structure are induced by DMSO and DMSO/2H2O mixtures. For highly structured proteins, such as myoglobin and concanavalin A, the infrared spectra point to a progressive destabilisation of the secondary structure until at moderate DMSO concentrations (around 0.33 mol fraction) intermolecular beta-sheet formation and aggregation are induced, as indicated by the appearance of a strong band at 1621 cm-1. This is a direct consequence of the disruption of intramolecular peptide group interactions by DMSO (partial unfolding). At higher DMSO concentrations (above 0.75 mol fraction), such aggregates are dissociated by disruption of the intermolecular C = O...2H-N deuterium bonds. The presence of a single amide I band at 1662 cm-1 corresponding to free amide C = O groups indicates that at high concentrations and in pure DMSO the proteins are completely unfolded, lacking any secondary structure. While low concentrations of DMSO showed no detectable effect upon the gross secondary structure of myoglobin and concanavalin A, the thermal stability of both proteins was markedly reduced. In alpha-casein, a highly unstructured protein, the situation is one of direct competition. The amide I maximum in 2H2O, at 1645 cm-1, is typical of unordered proteins with C = O groups deuterium-bonded predominantly to 2H2O. Addition of DMSO disrupts such interactions by competing with the peptide C = O group for the deuterium bond donor capacity of the 2H2O, and so progressively increases the amide I maximum until it stabilizes at 1663 cm-1, a position indicative of free C = O groups.     

N.m.r. study on conformation of Ac-Thr(alpha-GalNAc)-Ala-Ala-OMe as a model for mucin type glycoprotein

This study report on the results of high resolution 1H n.m.r. investigations on Ac-Thr(alpha-GalNAc)-Ala-Ala-OMe 1 as a mucin type model glycopeptide of antifreeze glycoprotein (AFGP) in both dimethyl sulfoxide (DMSO) and H2O. The temperature dependence of amide proton chemical shifts strongly suggested the presence of the intramolecular hydrogen bond between the amide proton of GalNAc and the carbonyl oxygen of the Thr residues. Due to this bond, the orientation of the sugar residue of 1 appears to be fairly restricted relative to its peptide backbone. Despite the lack of the clear evidence for such intramolecular hydrogen bond in H2O, 1H coupling constant data suggested the structural similarity of 1 in DMSO and H2O, indicating the presence of the intramolecular hydrogen bond even in H2O, which may play an important role in determining the orientation of the sugar moiety with respect to the peptide backbone in glycoprotein.     

Comparison of the conformation and electrostatic surface properties of magainin peptides bound to sodium dodecyl sulfate and dodecylphosphocholine micelles

The role played by noncovalent interactions in inducing a stable secondary structure onto the sodium dodecyl sulfate (SDS) and dodecylphosphocholine (DPC) micelle-bound conformations of (Ala(8,13,18))magainin 2 amide and the DPC micelle bound conformation of magainin 1 were determined. Two-dimensional NMR and molecular modeling investigations indicated that (Ala(8,13,18))magainin 2 amide bound to DPC micelles adopts a alpha-helical secondary structure involving residues 2-16. The four C-terminal residues converge to a lose beta-turn structure. (Ala(8,13,18))magainin 2 amide bound to SDS miscelles adopts a alpha-helical secondary structure involving residues 7-18. The C- and N-terminal residues exhibited a great deal of conformational flexibility. Magainin 1 bound to DPC micelles adopts a alpha-helical secondary structure involving residues 4-19. The C-terminal residues converge to a lose beta-turn structure. The results of this investigation indicate hydrophobic interactions are the major contributors to stabilizing the induced helical structure of the micelle-bound peptides. Electrostatic interactions between the polar head groups of the micelle and the cationic side chains of the peptides define the positions along the peptide backbone where the helical structures begin and end.     

NMR solution structure and membrane interaction of the N-terminal sequence (1-30) of the bovine prion protein

The structure and membrane interaction of the N-terminal sequence (1-30) of the bovine prion protein (bPrPp) has been investigated by NMR spectroscopy in phospholipid membrane mimetic systems. CD spectroscopy revealed that the peptide adopts a largely alpha-helical structure in zwitterionic bicelles as well as in DHPC micelles but has a less degree of alpha-helix structure in partly charged bicelles. The solution structure of bPrPp was determined in DHPC micelles, and an alpha-helix was found between residues Ser8 and Ile21. The residues within the helical region show slow amide hydrogen exchange. Translational diffusion measurements in zwitterionic q = 0.5 bicelles show that the peptide does not induce aggregation of the bicelles. Increased quadrupolar splittings were observed in the outer part of the (2)H spectrum of DMPC in q = 3.5 bicelles, indicating that the peptide induces a certain degree of order in the bilayer. The amide hydrogen exchange and the (2)H NMR results are consistent with a slight positive hydrophobic mismatch and that bPrPp forms a stable helix that inserts in a transmembrane location in the bilayer. The structure of bPrPp and its position in the membrane may be relevant for the understanding of how the N-terminal (1-30) part of the bovine PrP functions as a cell-penetrating peptide. These findings may lead to a better understanding of how the prion protein accumulates at the membrane surface and also how the conversion into the scrapie form is carried out.     

Native and non-native secondary structure and dynamics in the pH 4 intermediate of apomyoglobin

The partly folded state of apomyoglobin at pH 4 represents an excellent model for an obligatory kinetic folding intermediate. The structure and dynamics of this intermediate state have been extensively examined using NMR spectroscopy. Secondary chemical shifts, (1)H-(1)H NOEs, and amide proton temperature coefficients have been used to probe residual structure in the intermediate state, and NMR relaxation parameters T(1) and T(2) and ?(1)H?-(15)N NOE have been analyzed using spectral densities to correlate motion of the polypeptide chain with these structural observations. A significant amount of helical structure remains in the pH 4 state, indicated by the secondary chemical shifts of the (13)C(alpha), (13)CO, (1)H(alpha), and (13)C(beta) nuclei, and the boundaries of this helical structure are confirmed by the locations of (1)H-(1)H NOEs. Hydrogen bonding in the structured regions is predominantly native-like according to the amide proton chemical shifts and their temperature dependence. The locations of the A, G, and H helix segments and the C-terminal part of the B helix are similar to those in native apomyoglobin, consistent with the early, complete protection of the amides of residues in these helices in quench-flow experiments. These results confirm the similarity of the equilibrium form of apoMb at pH 4 and the kinetic intermediate observed at short times in the quench-flow experiment. Flexibility in this structured core is severely curtailed compared with the remainder of the protein, as indicated by the analysis of the NMR relaxation parameters. Regions with relatively high values of J(0) and low values of J(750) correspond well with the A, B, G, and H helices, an indication that nanosecond time scale backbone fluctuations in these regions of the sequence are restricted. Other parts of the protein show much greater flexibility and much reduced secondary chemical shifts. Nevertheless, several regions show evidence of the beginnings of helical structure, including stretches encompassing the C helix-CD loop, the boundary of the D and E helices, and the C-terminal half of the E helix. These regions are clearly not well-structured in the pH 4 state, unlike the A, B, G, and H helices, which form a native-like structured core. However, the proximity of this structured core most likely influences the region between the B and F helices, inducing at least transient helical structure.     

Conformational studies of human Des-Trp1,Nle12-minigastrin in water-trifluoroethanol mixtures by 1H NMR and circular dichroism

The 1H NMR spectrum of the title peptide, H-Leu-(Glu)5-Ala-Tyr-Gly-Trp-Nle-Asp-Phe-NH2, in 90% H2O/10% D2O was assigned by two-dimensional methods, and the displacement of the proton resonances upon addition of 2,2,2-trifluoroethanol (TFE) was followed. This permitted the assignment of the spectrum in 90% TFE/10% D2O. While the water conformation of the minigastrin analogue is random, the CD spectrum indicates that an ordered structure is present in TFE. Variable-temperature NMR data in this medium show that six amide protons have low temperature coefficients, two of the five Glu's, Trp, Nle, Asp, and Phe. These results were interpreted in terms of an alpha-helical stretch comprising the Leu and the five Glu residues and a 3(10)-helix initiated by a beta-turn at the sequence -Ala-Tyr-Gly-Trp-. Both CD and NMR data at different solvent compositions show two regions of conformational change, between 20 and 25% water and above 60% water.     

Conformational features of a hexapeptide model Ac-TGAAKA-NH2 corresponding to a hydrated alpha helical segment from glyceraldehyde 3-phosphate dehydrogenase: implications for the role of turns in helix folding

Recent analysis of alpha helices in protein crystal structures, available in literature, revealed hydrated alpha helical segments in which, water molecule breaks open helix 5-->1 hydrogen bond by inserting itself, hydrogen bonds to both C=O and NH groups of helix hydrogen bond without disrupting the helix hydrogen bond, and hydrogen bonds to either C=O or NH of helix hydrogen bond. These hydrated segments display a variety of turn conformations and are thought to be 'folding intermediates' trapped during folding-unfolding of alpha helices. A role for reverse turns is implicated in the folding of alpha helices. We considered a hexapeptide model Ac-1TGAAKA6-NH2 from glyceraldehyde 3-phosphate dehydrogenase, corresponding to a hydrated helical segment to assess its role in helix folding. The sequence is a site for two 'folding intermediates'. The conformational features of the model peptide have been investigated by 1H 2D NMR techniques and quantum mechanical perturbative configuration interaction over localized orbitals (PCILO) method. Theoretical modeling largely correlates with experimental observations. Based upon the amide proton temperature coefficients, the observed d alpha n(i, i + 1), d alpha n(i, i + 2), dnn(i, i + 1), d beta n(i, i + 1) NOEs and the results from theoretical modeling, we conclude that the residues of the peptide sample alpha helical and neck regions of the Ramachandran phi, psi map with reduced conformational entropy and there is a potential for turn conformations at N and C terminal ends of the peptide. The role of reduced conformational entropy and turn potential in helix formation have been discussed. We conclude that the peptide sequence can serve as a 'folding intermediate' in the helix folding of glyceraldehyde 3-phosphate dehydrogenase.     

Solution conformation of a model hexapeptide containing RGD sequence.

The solution conformation of a model hexapeptide Asp-Arg-Gly-Asp-Ser-Gly (DRGDSG) containing the RGD sequence has been studied in DMSO-d6 as well as in aqueous solution (H2O:D2O/90:10%) by 1H NMR spectroscopy. The unambiguous identification of spin systems of various amino acid residues and sequence specific assignment of all proton resonances was achieved by a combination of two dimensional COSY and NOESY experiments. The temperature coefficient data of the amide proton chemical shifts in conjunction with the vicinal coupling constants, i.e. 3JNH-C alpha H, NOESY and ROESY results indicate that the peptide in both the solvents exists in a blend of conformers with beta-sheet like extended backbone structure and folded conformations. The folded conformers do not appear to be stabilised by intramolecular hydrogen bonding. Our results are consistent with the flexibility of RGD segment observed in the NMR studies on the protein echistatin containing the RGD motif (references 23-25).     

Intrinsic helical propensities and stable secondary structure in a membrane-bound fragment (S4) of the shaker potassium channel.

The location and stability of helical secondary structure in a fragment comprising an extended sequence of the S4 transmembrane segment of the Shaker potassium channel was determined in methanol, and when bound to vesicles composed of egg phosphatidylcholine: egg phosphatidylglycerol (4:1; mol:mol) in water. The N-acetylated, C-amidated peptide corresponds to the sequence comprising residues A355-I384 in the Shaker potassium channel. Although NOEs characteristic of helical structure encompass essentially the full peptide sequence in methanol, analysis of amide and CH(alpha) chemical shifts, and amide exchange protection factors establish that stable helical structure comprises only around the first 22 amino acids of the 30 residue peptide. This sequence corresponds to that predicted to have the highest helical stability in water, indicating that while helical structure is considerably stabilised in methanol, the relative helical propensities of amino acids in methanol may be similar to those in water.In the presence of vesicles containing negatively charged lipids, helical structure corresponding to a maximum of around 40 % of the extended S4 peptide is induced; no helical structure is induced in the presence of vesicles composed only of neutral lipids. The location of stable helical structure in the membrane-bound peptide was determined by amide hydrogen-deuterium exchange trapping, and was shown to encompass the sequence between residues near M2 and I18. This sequence is similar to that having high helix propensity in water and methanol, supporting the idea that intrinsic helical propensities are important in defining the location of stable helical structure in polypeptides bound in the interfacial region of lipid bilayers. The study defines an approach to determining the location of, and contributions to, the stability of helical secondary structure in membrane-reconstituted polypeptides.     

Nuclear magnetic resonance determination of metal-proton distances in a synthetic calcium binding site of rabbit skeletal troponin C

The binding of gadolinium to a synthetic peptide of 13 amino acid residues representing the calcium binding loop of site 3 of rabbit skeletal troponin C [AcSTnC(103-115)amide] has been studied by using proton nuclear magnetic resonance (1H NMR) spectroscopy. In particular, the proton line broadening and enhanced spin-lattice relaxation have been used to determine proton-metal ion distances for several assigned nuclei in the peptide-metal ion complex. These distances have been used in conjunction with other constraints and a distance algorithm procedure to demonstrate that the structure of the peptide-metal complex as shown by 1H NMR is consistent with the structure of the EF calcium binding loop in the X-ray structure of parvalbumin but that the available 1H NMR distances do not uniquely define the solution structure.     

High-resolution mono- and multidimensional magic angle spinning 1H nuclear magnetic resonance of membrane peptides in nondeuterated lipid membranes and H2O.

High-speed (14 kHz) solid-state magic angle spinning (MAS) 1H NMR has been applied to several membrane peptides incorporated into nondeuterated dilauroyl or dimyristoylphosphatidylcholine membranes suspended in H2O. It is shown that solvent suppression methods derived from solution NMR, such as presaturation or jump-return, can be used to reduce water resonance, even at relatively high water content. In addition, regioselective excitation of 1H peptide resonances promotes an efficient suppression of lipid resonances, even in cases where these are initially two orders of magnitude more intense. As a consequence, 1H MAS spectra of the peptide low-field region are obtained without interference from water and lipid signals. These display resonances from amide and other exchangeable 1H as well as from aromatic nonexchangeable 1H. The spectral resolution depends on the specific types of resonance and membrane peptide. For small amphiphilic or hydrophobic oligopeptides, resolution of most individual amide resonance is achieved, whereas for the transmembrane peptide gramicidin A, an unresolved amide spectrum is obtained. Partial resolution of aromatic 1H occurs in all cases. Multidimensional 1H-MAS spectra of membrane peptides can also be obtained by using water suppression and regioselective excitation. For gramicidin A, F2-regioselective 2D nuclear Overhauser effect spectroscopy (NOESY) spectra are dominated by intermolecular through-space connectivities between peptide aromatic or formyl 1H and lipid 1H. These appear to be compatible with the known structure and topography of the gramicidin pore. On the other hand, for the amphiphilic peptide leucine-enkephalin, F2-regioselective NOESY spectra mostly display cross-peaks originating from though-space proximities of amide or aromatic 1H with themselves and with aliphatic 1H. F3-regioselective 3D NOESY-NOESY spectra can be used to obtain through-space correlations within aliphatic 1H. Such intrapeptide proximities should allow determination of the conformation of the peptide in membranes. It is suggested that high-speed MAS multidimensional 1H NMR of peptides in nondeuterated membranes and in H2O can be used for studies of both peptide structure and lipid-peptide interactions.