NMR and circular dichroic studies on the solution conformation of a synthetic peptide derived from the calmodulin-binding domain of Bordetella pertussis adenylate cyclase

The solution conformation of a synthetic peptide of 20 amino acids (P235-254) derived from the calmodulin-binding domain of Bordetella pertussis adenylate cyclase was studied by proton two-dimensional NMR spectroscopy and circular dichroism. Based on the standard techniques we have assigned all the resonances in the NMR spectrum to the corresponding protons of the peptide. Analysis of the secondary chemical shift distribution and of the nuclear Overhauser effect connectivities showed no evidence for a highly populated regular conformation but suggested the tendency to form an alpha-helix around the unique Trp residue. The propensity for a helical structure is in agreement with the results of circular dichroic spectroscopy showing a slight negative band at 222 nm which was cancelled by 6 M guanidine hydrochloride. Increasing amounts of 2,2,2-trifluoroethanol (up to 40%) increase considerably the helical population of the peptide as reflected in the circular dichroic spectra. Analysis of the present results shows that the free peptide P235-254 has the tendency to form a basic amphiphilic helix. The presence of two acid residues, Glu236 and Asp239, on the hydrophilic side of the alpha-helix, which is mainly composed by basic residues, may explain the lower affinity of this peptide for calmodulin as compared with other peptides derived from calmodulin-activated enzymes.     

Beyond the nearest-neighbor Zimm-Bragg model for helix-coil transition in peptides

The nearest-neighbor (micro = 1) variant of the Zimm and Bragg (ZB) model has been extensively used to describe the helix-coil transition in biopolymers. In this work, we investigate the helix-coil transition for a 21-residue alanine peptide (AP) with the ZB model up to fourth nearest neighbor (micro = 1, 2, 3, and 4). We use a matrix approach that takes into account combinations of any number of helical stretches of any length and therefore gives the exact statistical weight of the chain within the assumptions of the ZB model. The parameters of the model are determined by fitting the temperature-dependent circular dichroism and Fourier transform infrared experimental spectra of the AP. All variants of the model fit the experimental data, thus giving similar results in terms of the macroscopic observables, such as temperature-dependent fractional helicity. However, the resulting microscopic parameters, such as distributions of the individual residue helical probabilities and free energy surfaces, vary significantly depending on the variant of the model. Overall, the mean residue enthalpy and entropy (in the absolute value) both increase with micro, but combined yield essentially the same "effective" value of the ZB propagation parameters for all micro. Greater helical probabilities for individual residues are predicted for larger micro, in particular, near the center of the sequence. The ZB nucleation parameters increase with increasing micro, which results in a lower free energy barrier to helix nucleation and lower apparent "cooperativity" of the transition. The significance of the long-range interactions for the predictions of ZB model for helix-coil transition, the calculated model parameters and the limitations of the model are discussed.     

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]).     

Photo-control of peptide helix content by an azobenzene cross-linker: steric interactions with underlying residues are not critical

Photo-control of protein conformation could prove useful for probing function in diverse biological systems. Recently, we reported photo-switching of helix content in a short peptide containing an azobenzene cross-linker between cysteine residues at positions i and i + 7 in the sequence. In the original sequence, underlying residues at positions i + 3 and i + 4 were made bulky as preliminary modelling suggested that this would enhance photo-control of helix content. To test this hypothesis, peptides with Val, Aib; Ile, Aib; and Ala, Ala at positions i + 3 and i + 4 were synthesized, cross-linked and characterized. Before cross-linking, the peptides show distinct conformational behaviours: two with differing helix/coil mixtures whereas the other has a circular dichroism (CD) spectrum characteristic of beta-sheet and a tendency to aggregate. However, upon cross-linking the peptides have very similar CD spectra: predominantly random coil in the dark but predominantly helical upon irradiation. These results refute the original hypothesis. Steric interactions between the linker and underlying residues do not appear to be critical for photo-switching behaviour. When the cross-linking bridge is lengthened by replacing the i, i + 7 cysteine residues with homocysteine, a lower degree of photo-control of helicity is observed. Furthermore, a non-cross-linking version of the azobenzene reagent is shown not to produce any photo-control of helicity. We conclude that the intramolecular cross-link is essential for photo-switching and that it should be applicable to a wide range of peptides and proteins.     

Effect of the N3 residue on the stability of the alpha-helix

N3 is the third position from the N terminus in the alpha-helix with helical backbone dihedral angles. All 20 amino acids have been placed in the N3 position of a synthetic helical peptide (CH(3)CO-[AAX AAAAKAAAAKAGY]-NH(2)) and the helix content measured by circular dichroism spectroscopy at 273 K. The dependence of peptide helicity on N3 residue identity has been used to determine a free energy scale by analysis with a modified Lifson-Roig helix coil theory that includes a parameter for the N3 energy (n3). The most stabilizing residues at N3 in rank order are Ala, Glu, Met/Ile, Leu, Lys, Ser, Gln, Thr, Tyr, Phe, Asp, His, and Trp. Free energies for the most destabilizing residues (Cys, Gly, Asn, Arg, and Pro) could not be fitted. The results correlate with N1, N2, and helix interior energies and not at all with N-cap preferences. This completes our work on studying the structural and energetic preferences of the amino acids for the N-terminal positions of the alpha-helix. These results can be used to rationally modify protein stability, help design helices, and improve prediction of helix location and stability.     

What spectroscopy can still tell us about the secondary structure of bacteriorhodopsin.

The recently published model of the structure of bacteriorhodopsin (bR), developed by fitting the peptide chain to a high-resolution, three-dimensional density map, rules out the existence of transmembrane beta-sheet and provides an accurate estimate of the helix content. The precise geometry of the dihedral angles in the helical regions of the polypeptide cannot yet be specified from the diffraction data, however. Published data on the circular dichroism (CD) spectrum between 190 and 240 nm, and the infrared (IR) spectrum in the amide I band suggest that the helical conformation in bR may be, for the most part, a rather unusual one. The precise structural model, which specifies the number of residues in transmembrane helices, can now be used as an additional constraint in seeking models of the helical conformation that are in quantitative agreement with the CD and IR spectroscopic data. Further spectroscopic measurements can also be used to determine whether there are changes in the unusual dihedral-angle conformation within the helices during the photocycle.     

Synthetic α-helical peptides incorporating intercalators for DNA recognition

The design and synthesis of a water-soluble 14-residue peptide, in which a quinoline intercalator is attached to the peptide backbone via alkylation of a central cysteine residue, is reported. 600 MHz ¹H NMR spectroscopy and circular dichroism indicate that the peptide forms a nascent helix in aqueous solution, ie. an ensemble of turn-like structures over several adjacent residues in the peptide. A large number of sequential d_NN(i, i+1) connectivities were observed in NOESY spectra, and titration of trifluoroethanol into a solution of the peptide resulted in the characteristic CD spectrum expected for an α-helix. At low DNA concentrations, CD spectroscopy indicates that this helical conformation is stabilized, presumably due to folding of the peptide in the major groove of DNA.     

Helix propensities of the amino acids measured in alanine-based peptides without helix-stabilizing side-chain interactions.

Helix propensities of the amino acids have been measured in alanine-based peptides in the absence of helix-stabilizing side-chain interactions. Fifty-eight peptides have been studied. A modified form of the Lifson-Roig theory for the helix-coil transition, which includes helix capping (Doig AJ, Chakrabartty A, Klingler TM, Baldwin RL, 1994, Biochemistry 33:3396-3403), was used to analyze the results. Substitutions were made at various positions of homologous helical peptides. Helix-capping interactions were found to contribute to helix stability, even when the substitution site was not at the end of the peptide. Analysis of our data with the original Lifson-Roig theory, which neglects capping effects, does not produce as good a fit to the experimental data as does analysis with the modified Lifson-Roig theory. At 0 degrees C, Ala is a strong helix former, Leu and Arg are helix-indifferent, and all other amino acids are helix breakers of varying severity. Because Ala has a small side chain that cannot interact significantly with other side chains, helix formation by Ala is stabilized predominantly by the backbone ("peptide H-bonds"). The implication for protein folding is that formation of peptide H-bonds can largely offset the unfavorable entropy change caused by fixing the peptide backbone. The helix propensities of most amino acids oppose folding; consequently, the majority of isolated helices derived from proteins are unstable, unless specific side-chain interactions stabilize them.     

N(4)C-alkyl-N(4)C cross-linked DNA: bending deformations in duplexes that contain a -CNG- interstrand cross-link

Short DNA duplexes containing a 1,3-N(4)C-alkyl-N(4)C interstrand cross-link that joins the two C residues of a -CNG- sequence were prepared using either a phosphoramidite or convertible nucleoside approach. The alkyl cross-link consists of 2, 4, or 7 methylene groups. The duplexes, which contain a seven-base-pair core and A(3)/T(3) complementary 3'-overhanging ends, were characterized by enzymatic digestion and MALDI-TOF mass spectrometry. Ultraviolet thermal denaturation studies showed that the duplexes denature in a cooperative manner and that the length of the cross-link affects the thermal stability. Thus, the transition temperature of the ethyl cross-linked duplex, 42 degrees C, is 16 degrees C higher than the melting temperature of the corresponding non-cross-linked control, whereas the transition temperatures of the butyl and heptyl cross-linked duplexes, 73 and 72 degrees C, respectively, are 46-47 degrees C higher. The reduced molecularity of denaturation of the cross-linked duplexes versus melting of the non-cross-linked duplex most likely accounts for these differences. Examination of molecular models suggests that the ethyl cross-link is too short to span the distance between the two C residues at the site of the cross-link in B-form DNA without causing distortion of the helix, whereas less and no distortion would be expected for the butyl and heptyl cross-links, respectively. The circular dichroism spectra, which show greatest deviation in the ethyl cross-linked duplex from B-form DNA, are consistent with this expectation. Anomalous mobilities on native polyacrylamide gels of multimers produced by self-ligation of each of the cross-linked duplexes suggest that the ethyl and butyl cross-linked duplexes undergo bending deformations, whereas multimers derived from the heptyl cross-linked duplex migrated normally. The bending angle was estimated to be 20 degrees, 13 degrees, and 0 degrees for the ethyl, butyl, and heptyl cross-linked duplexes, respectively. Thus, it appears that the degree of bending in these N(4)C-alkyl-N(4)C cross-linked duplexes is controlled by the length of the cross-link.     

Protein engineering of a disulfide bond in a beta/alpha-barrel protein.

A disulfide bond has been introduced in the beta/alpha-barrel enzyme N-(5'-phosphoribosyl)anthranilate isomerase from Saccharomyces cerevisiae. The design of this disulfide bond was based on a model structure of this enzyme, built from the high-resolution crystal structure of the N-(5'-phosphoribosyl)anthranilate isomerase domain from Escherichia coli. The disulfide cross-link is spontaneously formed in vitro between residues 27 and 212, located in the structurally adjacent alpha-helices 1 and 8 of the outer helical ring of the beta/alpha-barrel. It creates a loop of 184 residues that account for 83% of the sequence of this enzyme, thus forming a quasi circular protein. The cross-linked mutant enzyme displays wild-type steady-state kinetic parameters. Measurements of the equilibrium constant for the reduction of this disulfide bond by 1,4-dithiothreitol show that its bond strength is comparable to that of other engineered protein disulfide bonds. The oxidized, cross-linked N-(5'-phosphoribosyl)anthranilate isomerase mutant is about 1.0 kcal/mol more stable than the wild-type enzyme, as estimated from its equilibrium unfolding transitions by guanidine hydrochloride.     

MEARA sequence repeat of human CstF-64 polyadenylation factor is helical in solution. A spectroscopic and calorimetric study.

The primary structure of the human CstF-64 polyadenylation factor contains 12 nearly identical repeats of a consensus motif of five amino acid residues with the sequence MEAR(A/G). No known function has yet been ascribed to this motif; however, according to secondary structure prediction algorithms, it should form a helical structure in solution. To validate this theoretical prediction, we synthesized a 31 amino acid residue peptide (MEARA(6)) containing six repeats of the MEARA sequence and characterized its structure and stability by circular dichroism (CD) spectroscopy and differential scanning calorimetry (DSC). No effects of concentration on the CD or DSC properties of MEARA(6) were observed, indicating that the peptide is monomeric in solution at concentrations up to 2 mM. The far UV-CD spectra of MEARA(6) indicates that at a low temperature (1 degrees C) the MEARA(6) peptide has a relatively high helical content (76% at pH 2.0 and 65% at pH 7.0). The effects of pH and ionic strength on the CD spectrum of MEARA(6) suggest that a number of electrostatic interactions (e.g., i, i + 3 Arg/Glu ion pair, charge-dipole interactions) contribute to the stability of the helical structure in this peptide. DSC profiles show that the melting of MEARA(6) helix is accompanied by positive change in the enthalpy. To determine thermodynamic parameters of helix-coil transition from DSC profiles for this peptide, we developed a new, semiempirical procedure based on the calculated function for the heat capacity of the coiled state for a broad temperature range. The application of this approach to the partial molar heat capacity function for MEARA(6) provides the enthalpy change for helix formation calculated per amino acid residue as 3.5 kJ/mol.     

Role of recurrent hydrophobic residues in catalysis of helix formation by T cell-presented peptides in the presence of lipid vesicles

We tested the hypothesis that the recurrence of hydrophobic amino acids in a polypeptide at positions falling in an axial, hydrophobic strip if the sequence were coiled as an alpha helix, can lead to helical nucleation on a hydrophobic surface. The hydrophobic surface could anchor such residues, whereas the peptide sequence grows in a helical configuration that is stabilized by hydrogen bonds among carbonyl and amido NH groups along the peptidyl backbone of the helix, and by other intercycle interactions among amino acid side chains. Such bound, helical structures might protect peptides from proteases and/or facilitate transport to a MHC-containing compartment and thus be reflected in the selection of T cell-presented segments. Helical structure in a series of HPLC-purified peptides was estimated from circular dichroism measurements in: 1) 0.01 M phosphate buffer, pH 7.0, 2) that buffer with 45% trifluoroethanol (TFE), and 3) that buffer with di-O-hexadecyl phosphatidylcholine vesicles. By decreasing the dielectric constant of the buffer, TFE enhances intrapeptide interactions generally, whereas the lipid vesicles only provide a surface for hydrophobic interactions. The peptides varied in their strip-of-helix hydrophobicity indices (SOHHI; the mean Kyte-Doolittle hydrophobicities of residues in an axial strip of an alpha helix) and in proline content. Structural order for peptides with helical circular dichroism spectra was estimated as percentage helicity from circular dichroism theta 222 nm values and peptide concentration. A prototypic alpha helical peptide with three cycles plus two amino acids and an axial hydrophobic strip of four leucyl residues (SOHHI = 3.8) was disordered in phosphate buffer, 58% helical in that buffer with 48% TFE, and 36% helical in that buffer with vesicles. Percentage helicity in the presence of vesicles of the subset of peptides without proline followed their SOHHI values. Peptides with multiple prolyl residues had circular dichroism spectra with strong signals, but since they did not have altered spectra in the presence of vesicles relative to phosphate buffer alone, the hydrophobic surface of the vesicle did not appear to stabilize those structures.     

Addition of side chain interactions to modified Lifson-Roig helix-coil theory: application to energetics of phenylalanine-methionine interactions.

We introduce here i, i + 3 and i, i + 4 side chain interactions into the modified Lifson-Roig helix-coil theory of Doig et al. (1994, Biochemistry 33:3396-3403). The helix/coil equilibrium is a function of initiation, propagation, capping, and side chain interaction parameters. If each of these parameters is known, the helix content of any isolated peptide can be predicted. The model considers every possible conformation of a peptide, is not limited to peptides with only a single helical segment, and has physically meaningful parameters. We apply the theory to measure the i, i + 4 interaction energies between Phe and Met side chains. Peptides with these residues spaced i, i + 4 are significantly more helical than controls where they are spaced i, i + 5. Application of the model yields delta G for the Phe-Met orientation to be -0.75 kcal.mol-1, whereas that for the Met-Phe orientation is -0.54 kcal.mol-1. These orientational preferences can be explained, in part, by rotamer preferences for the interacting side chains. We place Phe-Met i, i + 4 at the N-terminus, the C-terminus, and in the center of the host peptide. The model quantitatively predicts the observed helix contents using a single parameter for the side chain-side chain interaction energy. This result indicates that the model works well even when the interaction is at different locations in the helix.     

Effect of the N2 residue on the stability of the α-helix for all 20 amino acids

N2 is the second position in the alpha-helix. All 20 amino acids were placed in the N2 position of a synthetic helical peptide (CH(3)CO-[AXAAAAKAAAAKAAGY]-NH(2)) and the helix content was measured by circular dichroism spectroscopy at 273K. The dependence of peptide helicity on N2 residue identity has been used to determine a free-energy scale by analysis with a modified Lifson-Roig helix-coil theory that includes a parameter for the N2 energy (n2). The rank order of DeltaDeltaG((relative to Ala)) is Glu(-), Asp(-) > Ala > Glu(0), Leu, Val, Gln, Thr, Ile, Ser, Met, Asp(0), His(0), Arg, Cys, Lys, Phe > Asn, > Gly, His(+), Pro, Tyr. The results correlate very well with N2 propensities in proteins, moderately well with N1 and helix interior preferences, and not at all with N-cap preferences. The strongest energetic effects result from interactions with the helix dipole, which favors negative charges at the helix N terminus. Hydrogen bonds to side chains at N2, such as Gln, Ser, and Thr, are weak, despite occurring frequently in protein crystal structures, in contrast to the N-cap position. This is because N-cap hydrogen bonds are close to linear, whereas N2 hydrogen bonds have poor geometry. These results can be used to modify protein stability rationally, help design helices, and improve prediction of helix location and stability.     

Structural properties of a peptide derived from H-V-ATPase subunit a

The 3D structure of a peptide derived from the putative transmembrane segment 7 (TM7) of subunit a from H⁺-V-ATPase from Saccharomyces cerevisiae has been determined by solution state NMR in SDS. A stable helix is formed from L736 up to and including Q745, the lumenal half of the putative TM7. The helical region extends well beyond A738, as was previously suggested based on NMR studies of a similar peptide in DMSO. The pKa of both histidine residues that are important for proton transport was measured in water and in SDS. The differences that are found demonstrate that the histidine residues interact with the SDS polar heads. In detergent, circular dichroism data indicate that the secondary structure of the peptide depends on the pH and the type of detergent used. Using solid-state NMR, it is shown that the peptide is immobile in phospholipid bilayers, which means that it is probably not a single transmembrane helix in these samples. The environment is important for the structure of TM7, so in subunit a it is probably held in place by the other transmembrane helices of this subunit.     

NMR structure of human apolipoprotein C-II in the presence of sodium dodecyl sulfate

The structure and protein-detergent interactions of apolipoprotein C-II (apoC-II) in the presence of SDS micelles have been investigated using circular dichroism and heteronuclear NMR techniques applied to (15)N-labeled protein. Micellar SDS, a commonly used mimetic of the lipoprotein surface, inhibits the aggregation of apoC-II and induces a stable structure containing approximately 60% alpha-helix as determined by circular dichroism. NMR reveals the first 12 residues of apoC-II to be structurally heterogeneous and largely disordered, with the rest of the protein forming a predominantly helical structure. Three regions of helical conformation, residues 16-36, 50-56, and 63-77, are well-defined by NMR-derived constraints, with the intervening regions showing more loosely defined helical conformation. The structure of apoC-II is compared to that determined for other apolipoproteins in a similar environment. Our results shed light on the lipid interactions of apoC-II and its mechanism of lipoprotein lipase activation.     

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.     

Effect of the N1 residue on the stability of the alpha-helix for all 20 amino acids

N1 is the first residue in an alpha-helix. We have measured the contribution of all 20 amino acids to the stability of a small helical peptide CH(3)CO-XAAAAQAAAAQAAGY-NH(2) at the N1 position. By substituting every residue into the N1 position, we were able to investigate the stabilizing role of each amino acid in an isolated context. The helix content of each of the 20 peptides was measured by circular dichroism (CD) spectroscopy. The data were analyzed by our modified Lifson-Roig helix-coil theory, which includes the n1 parameter, to find free energies for placing a residue into the N1 position. The rank order for free energies is Asp(-), Ala > Glu(-) > Glu(0) > Trp, Leu, Ser > Asp(0), Thr, Gln, Met, Ile > Val, Pro > Lys(+), Arg, His(0) > Cys, Gly > Phe > Asn, Tyr, His(+). N1 preferences are clearly distinct from preferences for the preceding N-cap and alpha-helix interior. pK(a) values were measured for Asp, Glu, and His, and protonation-free energies were calculated for Asp and Glu. The dissociation of the Asp proton is less favorable than that of Glu, and this reflects its involvement in a stronger stabilizing interaction at the N terminus. Proline is not energetically favored at the alpha-helix N terminus despite having a high propensity for this position in crystal structures. The data presented are of value both in rationalizing mutations at N1 alpha-helix sites in proteins and in predicting the helix contents of peptides.     

A design approach to the structural analysis of interleukin-2

A semi-synthetic protein design approach has been employed for the structural investigation of a putative helical region at the C-terminus of Interleukin-2. With crystallographic or NMR derived conformational data as yet unavailable, we have relied only on primary sequence information and computer-assisted modelling to direct the analysis. By employing both chemical peptide synthesis and recombinant DNA methods, the C-terminus of IL-2 was modified according to a strategy designed to stabilize helical secondary structure. A semi-synthetic protein incorporating 12 simultaneous amino acid replacements was constructed, which possessed potentiated biological activity and displayed a far UV circular dichroism spectrum comparable to a hybrid protein with the authentic sequence. By comparison, another hybrid protein containing a C-terminal region designed to contain helix breaking residues was totally devoid of bioactivity. These findings provide evidence that the modelling method correctly identified a helix necessary for the formation of a bioactive tertiary fold. Moreover, by employing semi-synthesis it was possible to circumvent the difficulties associated with the preparation, purification and analysis of multiple recombinant proteins, and also to avoid the unreliability of total chemical synthesis for proteins greater than 100 residues.     

Solution structure of humanin, a peptide against Alzheimer's disease-related neurotoxicity

Humanin is a newly identified 24-residue peptide that suppresses neuronal cell death caused by a wide spectrum of familial Alzheimer's disease genes and the beta-amyloid peptide. In this study, NMR and circular dichroism studies of synthetic humanin in aqueous and 30% 2,2,2-trifluoroethanol (TFE) solutions are reported. In aqueous solution, humanin exists predominantly in an unstructured conformation in equilibrium with turn-like structures involving residues Gly5 to Leu10 and Glu15 to Leu18, providing indication of nascent helix. In the less polar environment of 30% TFE, humanin readily adopts helical structure with long-range order spanning residues Gly5 to Leu18. Comparative 3D modeling studies and topology predictions are in qualitative agreement with the experimental findings in both environments. Our studies reveal a flexible peptide in aqueous environment, which is free to interact with possible receptors that mediate its action, but may also acquire a helical conformation necessary for specific interactions and/or passage through membranes.