Conformational investigation of alpha,beta-dehydropeptides. XVI. Beta-turn tendency in Ac-Pro-DeltaXaa-NHMe: crystallographic and theoretical studies.

The crystal structures of two diastereomeric alpha,beta-dehydrobutyrine peptides Ac-Pro-(Z)-DeltaAbu-NHMe (I) and Ac-Pro-(E)-DeltaAbu-NHMe (II) have been determined. Both dehydropeptides adopt betaI-turn conformation characterized by the pairs of (phi(i+1), psi(i+1)) and (phi(i+2), psi(i+2)) angles as -66, -19, -97, 11 degrees for I and -59, -27, -119, 29 degrees for II. In each peptide, the betaI turn is stabilized by (i + 3) --> i intramolecular hydrogen bonds with N...O distance of 3.12 A for I and 2.93 A for II. These structures have been compared to the crystal structures of homologous peptides Ac-Pro-DeltaVal-NHMe and Ac-Pro-DeltaAla-NHMe. Theoretical analyses by DFT/B3LYP/6-31 + G** method of conformers formed by these four peptides and by the saturated peptide Ac-Pro-Ala-NHMe revealed that peptides with a (Z) substituent at the C(beta) (i+2) atom of dehydroamino acid, i.e. Ac-Pro-DeltaVal-NHMe and Ac-Pro-(Z)-DeltaAbu-NHMe, predominantly form beta turns, both in vacuo and in polar environment. The tendency to adopt beta-turn conformation is much weaker for the peptides lacking the (Z) substituent, Ac-Pro-(E)-DeltaAbu-NHMe and Ac-Pro-DeltaAla-NHMe. The latter adopts a semi-extended or an extended conformation in every polar environment, including a weakly polar solvent. The saturated peptide Ac-Pro-Ala-NHMe in vacuo prefers a beta-turn conformation, but in polar environment the differences between various conformers are small. The role of pi-electron correlation and intramolecular hydrogen bonds interaction in stabilizing the hairpin structures are discussed.     

Conformational investigation of alpha,beta-dehydropeptides. X. Molecular and crystal structure of Ac-DeltaAla-NMe2 compared with those of Ac-L-Ala-NMe2, Ac-DL-Ala-NMe2 and other dimethylamides.

A series of three homologous dimethyldiamides Ac-DeltaAla-NMe2, Ac-L-Ala-NMe2 and Ac-DL-Ala-NMe2 has been synthesized and the structures of these amides determined from single-crystal X-ray diffraction data. To learn more about the conformational preferences of compounds studied, the fully relaxed (phi-psi) conformational energy maps in vacuo (AM1) of Ac-DeltaAla-NMe2 and Ac-L-Ala-NMe2 were obtained, and the calculated minima reoptimized with the DFT/B3LYP/6-31G** method. The crystal-state results have been compared with the literature data. Ac-DeltaAla-NMe2 and other alpha,beta-dehydroamino acid dimethyldiamides, Ac-DeltaXaa-NMe2 adopt the conservative conformation of the torsion angles phi, psi = approximately -45 degrees, approximately 130 degrees, which are located in the high-energy region (region H) of Ramachandran diagram. Ac-L-Ala-NMe2 and Ac-DL-Ala-NMe2, as well as other saturated amino acid dimethylamides Ac-L/DL-Xaa-NMe2, present common peptide structures, and no conformational preferences are observed. Molecular packing of the amides analysed reveals two general hydrogen-bonded motifs. Dehydro and DL-species are paired into centrosymmetric dimers, and L-compounds form catemers. However, Ac-DeltaAla-NMe2 and Ac-DL-Ala-NMe2 constitute exceptions: their molecules also link into catemers.     

Conformational investigation of alpha, beta-dehydropeptides. XI. Molecular and crystal structure of Ac-(Z)-deltaPhe-NMe2 as compared to those of related molecules.

A series of three homologous dimethyldiamides Ac-(Z)-deltaPhe-NMe2, Ac-L-Phe-NMe2 and Ac-DL-Phe-NMe2 have been synthesized and their structures determined from single-crystal X-ray diffraction data. To learn more about the conformational preferences of the compounds studied, the fully relaxed phi, psi conformational energy maps on the free molecules of Ac-deltaAla-NMe2 and Ac-(Z)-deltaPhe-NMe2 were obtained with the HF/3-21G method and the calculated minima re-optimized with the DFT/B3LYP/6-31G** method. The crystal state results have been compared with the literature data. The studied dimethyldiamide Ac-deltaXaa-NMe2 combines the double bond in positions alpha, beta and the C-terminal tertiary amide within one molecule. As the representative probe with deltaXaa = deltaAla, (Z)-deltaLeu and (Z)-deltaPhe shows, in the solid state they adopt the conservative conformation with phi, psi approximately -45 degrees, approximately 130 degrees and with a non-planar tertiary amide bond, whatever the packing forces are. This conformation is located on the Ramachandran map in region H/F, which is of high-energy for common amino acids, but not so readily accessible to them. The free molecule calculations on Ac-deltaAla-NMe2 and Ac-(Z)-deltaPhe-NMe2 reveal that, in spite of dissimilar overall conformational profiles of these molecules, this structure is one of their low-energy conformers and for Ac-(Z)-deltaPhe-NMe2 it constitutes the global minimum. So, the theoretical results corroborate those experimental results proving that this structure is robust enough to avoid conformational distortion due to packing forces. In contrast to Ac-deltaXaa-NMe2, the saturated Ac-L/DL-Xaa-NMe2 shows the constancy of the associative patterns but do not prefer any molecular structure in the solid state.     

Conformational investigation of alpha,beta-dehydropeptides. N-acetyl-(E)-dehydrophenylalanine N'-methylamide: conformational properties from infrared and theoretical studies, part XIV.

N-Acetyl-(E)-dehydrophenylalanine N'-methylamide [Ac-(E)-DeltaPhe-NHMe], one of a few representative (E)-alpha,beta-dehydroamino acids, was studied by FTIR in dichloromethane and acetonitrile. To support spectroscopic interpretations and to gain some deeper insight into the Ac-(E)-DeltaPhe-NHMe molecule, the Ramachandran potential energy surface was calculated by the B3LYP/6-31G*//HF/3-21G method and the conformers localized were fully optimized at the B3LYP/6-31 + G** level. The spectra and calculations were compared with those of the related molecules Ac-DeltaAla-NHMe and Ac-(Z)-DeltaPhe-NHMe. The title compound assumes two conformational states in equilibrium in dichloromethane solution with a predominance of the extended conformer E. The Ac-(E)-DeltaPhe-NHMe spectrum is like that of Ac-DeltaAla-NHMe, particularly in the region of bands AI and AII, and unlike that of Ac-(Z)-DeltaPhe-NHMe. The positions of bands AI and II together with the nu(s)(N1--H1) band proves that the conformers E of both DeltaAla and (E)-DeltaPhe compounds are stabilized by the quite strong C5 hydrogen bonds N1--H1...O2. The same conclusion is drawn from the Ramachandran diagrams. The conformers E of both compounds are placed in the global minima and the gaps in energy order between them and the second conformer are large. The conformers E of DeltaAla and (E)-DeltaPhe, apart from the N1--H1...O2 hydrogen bond, show the Cbeta--H...O1 interaction, and Ac-(E)-DeltaPhe-NHMe displays the NH/pi interaction with the N2--H2 projecting in the first carbon atom of the phenyl ring. The C5 hydrogen bond is stronger in (E)-DeltaPhe than that in the DeltaAla compound. This is in agreement with interactions found in the calculated structures and can be explained by the influence of the phenyl ring in position (E). In acetonitrile, the molecule of Ac-(E)-DeltaPhe-NHMe loses its C5 hydrogen bond and becomes unfolded, whereas that of Ac-DeltaAla-NHMe does not vary practically. Adopting conformation E in a non-polar solvent seems to be a general feature of the (E)-DeltaXaa residues.     

Predominant torsional forms adopted by dipeptide conformers in solution: parameters for molecular recognition.

The present paper describes the predominant conformational forms adopted by dipeptides in aqueous solution. More than 50 dipeptides were subjected to conformational analysis using SYBYL Random Search. The resultant collections of conformers for individual dipeptides, for small groups with related side chain residues and for large groups of about 50 dipeptides were visualized graphically and analysed using a novel three-dimensional pseudo-Ramachandran plot. The distribution of conformers, weighted according to the percentage of each in the total conformer pool, was found to be restricted to nine main combinations of backbone psi (psi) and phi (phi) torsion angles. The preferred psi values were in sectors A7 (+150 degrees to +/-180 degrees), A10 (+60 degrees to +90 degrees) and A4 (-60 degrees to -90 degrees), and these were combined with preferred phi values in sectors B12 (-150 degrees to +/-180 degrees), B9 (-60 degrees to -90 degrees) and B2 (+30 degrees to +60 degrees). These combinations of psi and phi values are distinct from those found in common secondary structures of proteins. These results show that although dipeptides can each adopt many conformations in solution, each possesses a profile of common conformers that is quantifiable. A similarly weighted distribution of dipeptide conformers according to distance between amino-terminal nitrogen and carboxyl-terminal carbon shows how the preferred combinations of backbone torsional angles result in particular N-C geometries for the conformers. This approach gives insight into the important conformational parameters of dipeptides that provide the basis for their molecular recognition as substrates by widely distributed peptide transporters. It offers a basis for the rational design of peptide-based bioactive compounds able to exploit these transporters for targeting and delivery.     

Peptide inhibitors of E. collagenolyticum bacterial collagenase--effect of N-methylation. Consequences on biological activity and conformational properties.

Peptide inhibitors of E. collagenolyticum bacterial collagenase, HS-CH2-CH2-CO-Pro-Yaa (Yaa = Ala, Leu, Nle), have been N-methylated at the Yaa position. The N-methylation slightly increases the inhibitory potency of the modified peptides as compared to the parent compounds. The conformational effects of the N-methylation have been investigated by both 1H 2D-NMR and molecular mechanics energy minimization. Three low-energy conformers have been predicted for the unmethylated parent compounds (Yaa = Ala, Leu, Nle). They are characterized by the psi value of the central proline residue: psi Pro = 150 degrees (trans' conformation), psi Pro = 70 degrees (C7 conformation) and psi Pro = -50 degrees (cis' conformation). The N-methylation has been found to strongly increase the energy of the C7 conformer and to a less extent the energy of the cis' conformer. This leaves the trans' conformation as the only low-energy conformer. The ROESY experiments have established that both the N-methyl peptides and the parent compounds adopt the same preferred backbone conformation in water solution, i.e. the trans' conformation. Based on these results, the activities of the N-methyl peptides are discussed and a possible conformation of the inhibitor in the bound state is proposed.     

Significant conformational changes in an antigenic carbohydrate epitope upon binding to a monoclonal antibody.

Transferred nuclear Overhauser enhancement spectroscopy (TRNOE) was used to observe changes in a ligand's conformation upon binding to its specific antibody. The ligands studied were methyl O-beta-D-galactopyranosyl(1----6)-4-deoxy-4-fluoro-beta-D-galactopyra nos ide (me4FGal2) and its selectively deuteriated analogue, methyl O-beta-D-galactopyranosyl(1----6)-4-deoxy-2-deuterio-4-fluoro-beta -D- galactopyranoside (me4F2dGal2). The monoclonal antibody was mouse IgA X24. The solution conformation of the free ligand me4F2dGal2 was inferred from measurements of vicinal 1H-1H coupling constants, long-range 1H-13C coupling constants, and NOE cross-peak intensities. For free ligand, both galactosyl residues adopt a regular chair conformation, but the NMR spectra are incompatible with a single unique conformation of the glycosidic linkage. Analysis of 1H-1H and 1H-13C constants indicates that the major conformer has an extended conformation: phi = -120 degrees; psi = 180 degrees; and omega = 75 degrees. TRNOE measurements on me4FGal2 and me4F2dGal2 in the presence of the specific antibody indicate that the pyranose ring pucker of each galactose ring remains unchanged, but rotations about the glycosidic linkage occur upon binding to X24. Computer calculations indicate that there are two sets of torsion angles that satisfy the observed NMR constraints, namely, phi = -152 +/- 9 degrees; psi = -128 +/- 7 degrees; and omega = -158 +/- 6 degrees; and a conformer with phi = -53 +/- 6 degrees; psi = 154 +/- 10 degrees; and omega = -173 +/- 6 degrees. Neither conformation is similar to any of the observed conformations of the free disaccharide.(ABSTRACT TRUNCATED AT 250 WORDS)     

Influence of N-terminal residue stereochemistry on the prolyl amide geometry and the conformation of 5-tert-butylproline type VI beta-turn mimics.

The effects of N-terminal amino acid stereochemistry on prolyl amide geometry and peptide turn conformation were investigated by coupling both L- and D-amino acids to (2S, 5R)-5-tert-butylproline and L-proline to generate, respectively, N-(acetyl)dipeptide N'-methylamides 1 and 2. Prolyl amide cis- and trans-isomers were, respectively, favored for peptides 1 and 2 as observed by proton NMR spectroscopy in water, DMSO and chloroform. The influence of solvent composition on amide proton chemical shift indicated an intramolecular hydrogen bond between the N'-methylamide proton and the acetamide carbonyl for the major conformer of dipeptides (S)-1, that became less favorable in (R)-1 and 2. The coupling constant (3J(NH,alpha)) values for the cis-isomer of (R)-1 indicated a phi2 dihedral angle value characteristic of a type VIb beta-turn conformation in solution. X-ray crystallographic analysis of N-acetyl-D-leucyl-5-tert-butylproline N'-methylamide (R)-lb showed the prolyl residue in a type VIb beta-turn geometry possessing an amide cis-isomer and psi3-dihedral angle having a value of 157 degrees, which precluded an intramolecular hydrogen bond. Intermolecular hydrogen bonding between the leucyl residues of two turn structures within the unit cell positioned the N-terminal residue in a geometry where their phi2 and psi2 dihedral angle values were not characteristic of an ideal type VIb turn. The circular dichroism spectra of tert-butylprolyl peptides (S)- and (R)-1b were found not to be influenced by changes in solvent composition from water to acetonitrile. The type B spectrum exhibited by (S)-1b has been previously assigned to a type VIa beta-turn conformation [Halab L, Lubell WD. J. Org. Chem. 1999; 64: 3312-3321]. The type C spectrum exhibited by the (R)-lb has previously been associated with type II' beta-turn and alpha-helical conformations in solution and appears now to be also characteristic for a type VIb geometry.     

Conformational features of C-glycosyl compounds: crystal structure and molecular modelling of "methyl C-gentiobioside"

The crystal of "methyl C-gentiobioside" (methyl 8,12-anhydro-6,7-dideoxy-D-glycero-D-gulo-alpha-D-gluco-trideca pyranoside) (C14H26O10) is triclinic, space group P1, with a = 1.0181 (6) nm, b = 0.8093 (5) nm, c = 0.5066 (4) nm, alpha = 96.03 (5) degrees, beta = 99.94 (5) degrees, gamma = 90.85 (5) degrees. The two D-glucose residues have the 4C1 conformation. The orientation of the beta-(1----6) linkage is characterized by torsion angles phi = 55.9 degrees, psi = 175.1 degrees, and omega = -63.9 degrees. The orientation of the primary hydroxyl group at the non-reducing residue is gauche-trans (omega' = -53.6 degrees). There is no intramolecular hydrogen bond. Molecules are held together by a network of hydrogen bonds involving all of the hydroxyl groups. This crystal structure is the first experimental characterization of a "C-disaccharide". Unlike methyl gentiobioside, which has a high level of conformational flexibility, the "C-disaccharide" has a restricted flexibility. Each of the low-energy conformers in vacuo has a value of phi centered about 60 degrees, in agreement with the solid state conformation, and the exo-anomeric effect is no longer predominant.     

Characterization of beta-turn and Asx-turns mimicry in a model peptide: stabilization via C--H . . . O interaction

The chemical synthesis and single-crystal X-ray diffraction analysis of a model peptide, Boc-Thr-Thr-NH2 (1) comprised of proteinogenic residues bearing an amphiphilic Cbeta -stereogenic center, has been described. Interestingly, the analysis of its molecular structure revealed the existence of a distinct conformation that mimics a typical beta-turn and Asx-turns, i.e., the two Thr residues occupy the left- and right-corner positions. The main-chain torsion angles of the N- and C-terminal residues i.e., semiextended: phi = -68.9 degrees , psi = 128.6 degrees ; semifolded: phi = -138.1 degrees , psi = 2.5 degrees conformations, respectively, in conjunction with a gauche- disposition of the obligatory C-terminus Thr CgammaH3 group, characterize the occurrence of the newly described beta-turn- and Asx-turns-like topology. The preferred molecular structure is suggested to be stabilized by an effective nonconventional main-chain to side-chain Ci=O . . . H--Cgamma(i+2)-type intraturn hydrogen bond. Noteworthy, the observed topology of the resulting 10-membered hydrogen-bonded ring is essentially similar to the one perceived for a classical beta-turn and the Asx-turns, stabilized by a conventional intraturn hydrogen bond. Considering the signs as well as magnitudes of the backbone torsion angles and the orientation of the central peptide bond, the overall mimicked topology resembles the type II beta-turn or type II Asx-turns. An analysis of Xaa-Thr sequences in high-resolution X-ray elucidated protein structures revealed the novel topology prevalence in functional proteins (unpublished). In view of indubitable structural as well as functional importance of nonconventional interactions in bioorganic and biomacromolecules, we intend to highlight the participation of Thr CgammaH in the creation of a short-range C=O . . . H--Cgamma -type interaction in peptides and proteins.     

Designing of peptides with left handed helical structure by incorporating the unusual amino acids

The conformational behaviour of delta Ala has been investigated by quantum mechanical method PCILO in the model dipeptide Ac-delta Ala-NHMe and in the model tripeptides Ac-X-delta Ala-NHMe with X = Gly, Ala, Val, Leu, Abu and Phe and is found to be quite different. The computational results suggest that in the model tripeptides the most stable conformation corresponds to phi 1 = -30 degrees, psi 1 = 120 degrees and phi 2 = psi 2 = 30 degrees in which the > C = 0 of the acetyl group is involved in hydrogen bond formation with N-H of the amide group. Similar results were obtained for the conformational behaviour of D-Ala in Ac-D-Ala-NHMe and Ac-Ala-D-Ala-NHMe. The conformational behaviour of the amino acids delta Ala, D-Ala, Val and Aib in model tripeptides have been utilized in the designing of left handed helical peptides. It is shown that the peptide HCO-(Ala-D-Ala)3-NHMe can adopt both left and right handed helix whereas in the peptide Ac-(Ala-delta Ala)3-NHMe the lowest energy conformer is beta-bend ribbon structure. Left handed helical structure with phi = 30 degrees, psi = 60 degrees for D-Ala residues and phi = psi = 30 degrees for delta Ala is found to be more stable by 4 kcal mole-1 than the corresponding right handed helical structure for the peptide Ac-(D-Ala-delta Ala)3-NHMe. In both the peptides Ac-(Val-delta Ala)3-NHMe and Ac-(D-Val-delta Ala)3-NHMe the most stable conformer is the left handed helix. Comparisons of results for Ac-(Ala-delta Ala)3-NHMe and Ac(Val-delta Ala)3-NHMe and Ac-(D-Ala-delta Ala)3-NHMe and Ac-(D-Val-delta Ala)3-NHMe also reveal that the Val residues facilitate the population of 3(10) left handed helix over the other conformers. It is also shown that the conformational behaviour of Aib residue depends on the chirality of neighbouring amino acids, i.e. Ac-(Aib-Ala)3-NHMe adopts right handed helical structure whereas Ac-(Aib-D-Ala)3-NHMe is found to be in left handed helical structure.     

DFT studies of the disaccharide, alpha-maltose: relaxed isopotential maps

The disaccharide, alpha-maltose, forms the molecular basis for the analysis of the structure of starch, and determining the conformational energy landscape as the molecule oscillates around the glycosidic bonds is of importance. Thus, it is of interest to determine, using density functionals and a medium size basis set, a relaxed isopotential contour map plotted as a function of the phi(H) and psi(H) dihedral angles. The technical aspects include the method of choosing the starting conformations, the choice of scanning step size, the method of constraining the specific dihedral angles, and the fitting of data to obtain well defined contour maps. Maps were calculated at the B3LYP/6-31+G( *) level of theory in 5 degrees intervals around the (phi(H),psi(H))=(0 degrees ,0 degrees ) position, out to approximately +/-30 degrees or greater, for gg-gg'-c, gg-gg'-r, gt-gt'-c, gt-gt'-r, tg-tg'-c, and tg-tg'-r conformers, as well as one-split gg(c)-gg'(r) conformer. The results show that the preferred conformation of alpha-maltose in vacuo depends strongly upon the hydroxyl group orientations ('c'/'r'), but the energy landscape moving away from the minimum-energy position is generally shallow and transitions between conformational positions can occur without the addition of significant energy. Mapped deviations of selected parameters such as the dipole moment; the C1-O1-C4', H1-C1-O1, and H4'-C4'-O1 bond angles; and deviations in hydroxymethyl rotamers, O5-C5-C6-O6, O5'-C5'-C6'-O6', C5-C6-O6-H, and C5'-C6'-O6'-H', are presented. These allow visualization of the structural and energetic changes that occur upon rotation about the glycosidic bonds. Interactions across the bridge are visualized by deviations in H(O2)...O3', H(O3')...O2, and H1...H4' distances and the H(O2)-O2-C2-C1 and H'(O3')-O3'-C3'-C4' hydroxyl dihedral angles.     

Design of peptides: synthesis, crystal structure, molecular conformation, and conformational calculations of N-Boc-L-Phe-Dehydro-Ala-OCH3.

It is noteworthy that the dehydro-Ala residue adopts an extended conformation that is different than those observed in dehydro-Phe, dehydro-Leu, and dehydro-Abu. The peptide N-Boc-L-Phe-dehydro-Ala-OCH3 (C18H24N2O5) was synthesized by the usual workup procedure and finally by converting N-Boc-L-Phe-L-Ser-OCH3 to N-Boc-L-Phe-dehydro-Ala- OCH3. It was crystallized from its solution in a methanol-water mixture at room temperature. The crystals belong to the monoclonic space group P2(1), with a = 9.577(1) A, b = 5.195(3) A, c = 19.563(3) A, beta = 94.67(5) degrees, V = 970.1(6) A3, Z = 2, dm = 1.201(5) Mg m-3, dc = 1.197(5) Mg m-3. The structure was determined using direct method procedures. It was refined by a full-matrix least-squares procedure to an R value of 0.048 for 1370 observed reflections. The C2 alpha-C2 beta distance is 1.327(8) A, while the bond angles N2-C2 alpha-C2' and C1'-N2-C2 alpha are 109.8(5) degrees and 127.8(5) degrees, respectively. The backbone adopts a nonspecific conformation with dehydro-Ala in a fully extended conformation with the following torsion angles: theta 1 = 175.2(4) degrees, omega 0 = 170.2(4) degrees, phi 1 = 135.8(5) degrees, psi 1 = -22.6(6) degrees, omega 1 = 168.5(5) degrees, phi 2 = -170.3(5) degrees, psi 2T = -178.6(5) degrees, theta T = 178.4(7) degrees. The rigid planar and trans conformation of dehydro-Ala forces Phe to adopt a strained conformation. The Boc group has a trans-trans conformation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Synthesis, crystal structure, and molecular conformation of N-Ac-dehydro-Phe-L-Val-L-Val-OCH3.

The peptide N-Ac-dehydro-Phe-L-Val-L-Val-OCH3 (C22H31N3O5) was synthesized by the usual workup procedure and finally by coupling the N-Ac-dehydro-Phe-L-Val-OH to valine methyl ester. It was crystallized from its solution in acetonitrile-water mixture at 4 degrees C. The crystals belong to the space group P1 with a = 8.900(3) A, b = 11.135(2) A, c = 12.918(2) A, alpha = 90.36(1) degrees, beta = 110.14(3) 14(3) degrees, V = 1207.7(6) A, 3Z = 2, dm = 1.156(5) Mgm-3, dc = 1.148(5) Mgm-3. The structure was determined by direct methods using SHELXS86. The structure was refined by full-matrix least-squares procedure to an R value of 0.077 for 3916 observed reflections. The molecular dimensions and conformations of the two crystallographically independent molecules are in good agreement. In the dehydro residues, the average C alpha-C beta distance is 1.31(2) A whereas the bond angle C alpha-C beta-C gamma is 132(1) degrees. The average backbone torsion angles are omega 0 = 169(1) degrees, phi 1 = -40(1) degree, psi 1 = -50(1) degree, omega 1 = -177(1) degree, phi 2 = 54(1) degree, psi 2 = 46(1) degree, omega 2 = -174(1) degree, phi 3 = 103(1) degree, psi T3 = -139(1) degree, and theta T3 = -176(1) degree. The acetyl group is in the trans conformation, while the backbone adopts a right-handed and left-handed helical conformation alternatingly.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of lengthening of peptide backbone by insertion of chiral beta-homo amino acid residues: conformational behavior of linear peptides containing alternating L-leucine and beta-homo L-leucine residues

The synthesis and the solution behavior of the linear peptides containing a beta-homo (beta-H) leucine residue-Boc-Leu-beta-HLeu-Leu-OMe, Boc-beta-HLeu-Leu-beta-HLeu-Leu-OMe, and Boc-Leu-beta-HLeu-Leu-beta-HLeu-Leu-OMe-as well as the solid structure of the tripeptide, are reported. The conformational behavior of the peptides was investigated in solution by two-dimensional nmr. Our data support the existence in solution with different families of conformers in rapid interchange. The crystals of the tripeptide are orthorhombic, space group P2(1)2(1)2, with a = 15.829(1) A, b = 29.659(1) A, c = 6.563(1) A, and Z = 4. The structure has been solved by direct methods and refined to final R1 and wR2 indexes of 0.0530 and 0.1436 for 2420 reflections with I > 2sigma(I). In the solid state, the tripeptide does not present intramolecular H bonds, and the peptide backbone of the two leucine residues adopts a quasi-extended conformation. For the beta-HLeu residue, the backbone conformation is specified by the torsion angles straight phi(2) = -120.9(4) degrees, mu(2) = 56.7(4) degrees, psi(3) = -133.2(4) degrees. The side chains of the three residues assume the same conformation (g(-), g(-), trans), and all peptide bonds, except the urethane group at the N-terminus, are in the trans conformation. Preliminary conformational energy calculations carried out on the Ac-NH-beta-HAla-NHMe underline that the conformations with mu angle equal to 180 degrees and 60 degrees assume lower energy with respect to the others. In addition, we found a larger conformational freedom for the psi angle with respect to the straight phi angle.     

Empirical torsional potential functions from protein structure data. Phi- and psi-potentials for non-glycyl amino acid residues.

The torsional potential functions Vt(phi) and Vt(psi) around single bonds N--C alpha and C alpha--C, which can be used in conformational studies of oligopeptides, polypeptides and proteins, have been derived, using crystal structure data of 22 globular proteins, fitting the observed distribution in the (phi, psi)-plane with the value of Vtot(phi, psi), using the Boltzmann distribution. The averaged torsional potential functions, obtained from various amino acid residues in L-configuration, are Vt(phi) = 1.0 cos (phi + 60 degrees); Vt(psi) = 0.5 cos (psi + 60 degrees) - 1.0 cos (2 psi + 30 degrees) - 0.5 cos (3 psi + 30 degrees). The dipeptide energy maps Vtot(phi, psi) obtained using these functions, instead of the normally accepted torsional functions, were found to explain various observations, such as the absence of the left-handed alpha helix and the C7 conformation, and the relatively high density of points near the line psi = 0 degrees. These functions derived from observational data on protein structures, will, it is hoped, explain various previously unexplained facts in polypeptide conformation.     

Crystal structure, conformation, and potential energy calculations of the chemotactic peptide N-formyl-L-Met-L-Leu-L-Phe-OMe

The tripeptide N-formyl-L-Met-L-Leu-L-Phe-OMe (FMLP-OMe) crystallizes in the orthorhombic system, space group P 2(1)2(1)2(1), with the following unit-cell parameters: a = 21.727, b = 21.836, c = 5.133 A, Z = 4. The structure has been solved and refined to a final R of 0.068 for 1838 independent reflexions with I greater than 2 omega (I). The peptide backbone is folded at the Leu residue (phi L = -67.7, psi L = -49.1 degrees) without intramolecular hydrogen bonds. Considering each peptide plane, the Leu side-chain is oriented on the same side of that of the Phe residue and on the opposite side of that of the Met residue, respectively. The crystal conformation differs from all the other conformations proposed for FMLP-OMe and the anionic form of N-formyl-L-Met-L-Leu-L-Phe-OH (FMLP) in solution accounts for the amphiphilic character of the peptide, giving rise, through intermolecular hydrogen bonds, to a stacking of molecules which could be maintained in the aggregation states experimentally observed in solvents of low polarity. Intramolecular potential energy calculations have been carried out in order to compare the energies of the various backbone conformers.     

Studies on the molecular recognition of synthetic methyl beta-lactoside analogs by ricin, a cytotoxic plant lectin

The binding of methyl beta-lactoside and of all possible monodeoxy derivatives of methyl beta-lactoside to the galactose-specific highly cytotoxin lectin ricin, has been investigated. The distribution of low-energy conformers of the disaccharide structures has been first determined using molecular-mechanics calculations and high-resolution NMR spectroscopy. The nuclear Overhauser enhancements and specific deshieldings observed are in agreement with a similar distribution of low-energy conformers for all studied compounds which may be described by a major conformer defined by phi (H1'-C1'-O1'-C4) and psi (C1'-O1'-C4-H4) torsion angles of 49 degrees and 5 degrees, respectively, with contribution of conformers with angles phi/psi 24 degrees/-59 degrees, 22 degrees/-32 degrees and 6 degrees/-44 degrees. Assuming that the disaccharides bind to the lectin in these preferred conformations, the apparent dissociation constants for the ricin-disaccharide complexes have been interpreted in terms of specific polar and nonpolar interactions. In agreement with X-ray data, the hydroxyl groups at positions 3, 4 and 6 of the beta-D-galactopyranose moiety appear as key polar groups in the interaction with ricin. These results are in contrast to previous results which have established that position 6 is not involved in lectin binding. An important nonpolar interaction involving position 3 of the beta-D-glucopyranose moiety, seems to be operative. The distribution of low-energy conformers of these disaccharide structures permits this interaction to take place with the hydroxyl group at this position intramolecularly bonded, thus rendering this region of the molecule more lipophylic in character for acceptance into nonpolar regions of the combining site.     

Conformational investigation of alpha, beta-dehydropeptides. Part III. Molecular and crystal structure of acetyl-L-prolyl-alpha, beta-dehydrovaline methylamide.

The crystal structure of Ac-Pro-delta Val-NHCH3 was examined to determine the influence of the alpha,beta-dehydrovaline residue on the nature of peptide conformation. The peptide crystallizes from methanol-diethyl ether solution at 4 degrees in needle-shaped form in orthorhombic space group P2(1)2(1)2(1) with a = 11.384(2) A, b = 13.277(2) A, c = 9.942(1) A, V = 1502.7(4) A3, Z = 4, Dm = 1.17 g.cm-3 and Dc = 1.18 g.cm-3. The structure was solved by direct methods using SHELXS-86 and refined to an R value of 0.057 for 1922 observed reflections. The peptide is found to adopt a beta-bend between the type I and the type III conformation with phi 1 = -68.3(4) degrees, psi 1 = -20.1(4) degrees, phi 2 = -73.5(4) degrees and psi 2 = -14.1(4) degrees. An intramolecular hydrogen bond between the carbonyl oxygen of ith residue and the NH of (i + 3)th residue stabilizes the beta-bend. An additional intermolecular N...O hydrogen bond joins molecules into infinite chains. In the literature described crystal structures of peptides having a single alpha,beta-dehydroamino acid residue in the (i + 2) position and forming a beta-bend reveal a type II conformation.     

A sequence preference for nucleation of alpha-helix--crystal structure of Gly-L-Ala-L-Val and Gly-L-Ala-L-Leu: some comments on the geometry of leucine zippers

The synthetic peptide Gly-L-Ala-L-Val (C10H19N3O4.3H2O; GAV) crystallizes in the monoclinic space group P21, with a = 8.052(2), b = 6.032(2), c = 15.779(7) A, beta = 98.520(1) degree, V = 757.8 A3, Dx = 1.312 g cm-3, and Z = 2. The peptide Gly-L-Ala-L-Leu (C11H21N3O4.3H2O; GAL) crystallizes in the orthorhombic space group P212121, with a = 6.024(1), b = 8.171(1), c = 32.791(1) A, V = 1614 A3, Dx = 1.289 g cm-3, and Z = 4. Their crystal structures were solved by direct methods using the program SHELXS-86, and refined to an R index of 0.05 for 1489 reflections for GAV and to an R index of 0.05 for 1563 reflections for GAL. The tripeptides exist as a zwitterion in the crystal and assume a near alpha-helical backbone conformation with the following torsion angles: psi 1 = -150.7 degrees; phi 2, psi 2 = -68.7 degrees, -38.1 degrees; phi 3, psi 32 = -74.8 degrees, -44.9 degrees, 135.9 degrees for GAV; psi 1 = -150.3 degrees; phi 2, psi 2 = -67.7 degrees, -38.9 degrees; phi 3, psi 31, psi 32 = -72.2 degrees, -45.3 degrees, 137.5 degrees for GAL. Both the peptide units in both of the tripeptides show significant deviation from planarity [omega 1 = -171.3(6) degrees and omega 2 = -172.0(6) degrees for GAV; omega 1 = -171.9(5) degrees and omega 2 = -173.2(6) degrees for GAL]. The side-chain conformational angles chi 21 and chi 22 are -61.7(5) degrees and 175.7(5) degrees, respectively, for valine, and the side-chain conformations chi 12 and chi 23's are -68.5(5) degrees and (-78.4(6) degrees, 159.10(5) degrees) respectively, for leucine. Each of the tripeptide molecule is held in a near helical conformation by a water molecule that bridges the NH3+ and COO- groups, and acts as the fourth residue needed to complete the turn by forming two hydrogen bonds. Two other water molecules form intermolecular hydrogen bonds in stabilizing the helical structure so that the end result is a column of molecules that looks like an alpha-helix.