Influence of the peptide chain length on the stability of double-stranded β-helical species of D,L-alternating oligovalines in chloroform solution

The type and distribution of the β-helixes occurring in chloroform solutions of Boc-(L-Val-D-Val)₆-OMe and Boc-(L-Val-D-Val)₈-OMe have been studied by using ¹H-nmr techniques. Right- and left-handed ↑↓β^4.4-helices and left-handed β^5.6-helices occur with the dodecapeptide. β^4.4-Helices of opposite handedness occur also with the hexadecapeptide, but ↑↓β^5.6-helices could not be detected with this oligomer. At equilibrium, at 25°C, the double helix of the dodecapeptide is only moderately populated. These results indicate that increasing the chain length has a destabilizing effect on the ↑↓β^5.6-helices of D ,L -alternating oligovalines in chloroform solution.     

15N-nmr spectroscopy. 33. Assignments of isotactic and syndiotactic sequences in poly(D,L-amino acids)

¹⁵N-enriched (D ,L -Leu)_n, (γ-OMe-D ,L -Glu)_n, (D ,L -Val)_n, and (D ,L -Phe)_n were prepared, 40.55-MHz ¹⁵N-nmr spectra were measured in various solvents. The signal patterns depend strongly on the nature of the solvent, yet in most cases at least four signals are resolved, representing the four enantiomeric pairs of triads L -L -L (D -D -D ), L -D -L (D -L -D ), L -L -D (D -D -L ), and D -L -L (L -D -D ). Numerous copolypeptides of the general structure (A)_n-B*-(A)_m (the asterisk denotes 40–50% ¹⁵N enrichment) were synthesized and measured as models for syndiotactic sequences in the spectra of poly(D ,L -amino acids). In this way unambiguous assignments for both isotactic and syndiotactic trials were obtained. A spectroscopic rule was established: “isotactic sequences absorb downfield of syndiotactic ones.” Furthermore, the spectra of various types of stereocopolypeptides such as (L -Leu/L -Val)_n and (L -Leu/D -Val)_n were investigated, including the ternary systems (L -Leu/L -Ala/D -Ala)_n (L -Leu/L -Ala/Gly)_n, (L -Leu/D -Ala/Gly)_n, (L -Val/L -Ala/Gly)_n, and (L -Val/D -Ala/Gly)_n. All copolymerization of D - and L -amino acid NCAs investigated in this work showed a low degree of stereoselectivity.     

Experimental investigations on the backbone folding of proline-containing model tripeptides

Some proline-containing tripeptides with the general formulas R⁰CO-L -Pro-X-NHR³ (X = Gly,Sar,L -Ala,D -Ala) and R⁰CO-X-L -Pro-NHR³ (X = Gly,L -Ala,D -Ala) have been investigated in solution by ir and ¹H-nmr spectroscopies. Their favored conformational states depend mainly on both the primary structure and the chiral sequence of the molecules. In inert solvents the βII-folding mode is the most favored conformation for the L -Pro-D -Ala and L -Pro-Gly tripeptides, while the βII′-turn is largely preferred by D -Ala-L -Pro derivatives. Under the same conditions only about one-third of the whole conformers of L -Pro-L -Ala molecules adopts the βI-folding mode. Semiopened C₇C₅ and C₅C₇ conformations are appreciably populated in the L -Pro-L -Ala sequence, on the one hand, and in the Gly-L -Pro and L -Ala-L -Pro derivatives, on the other hand. In L -Pro-Sar and X-L -Pro models, the cis–trans isomerism around the middle tertiary amide function is observed. Thus cis L -Pro-Sar and L -Ala-L -Pro conformers are folded by an intramolecular i + 3 → i hydrogen bond, whereas cis D -Ala-L -Pro and Gly-L -Pro molecules accommodate an open conformation. In dimethylsulfoxide the βII- and βII′-folding modes are not essentially destabilized, as contrasted with the βI conformation, which is less populated. In water solution all the above-mentioned conformations, with the possible exception of the βII′-folding mode for D -Ala-L -Pro molecules, seem to vanish. Solute conformations are also compared with the crystal structures of four proline-containing tripeptides.     

β-Turn conformations in crystal structures of model peptides containing α,α-Di-n-propylglycine and α,α-Di-n-butylglycine

The crystal state conformations of three peptides containing the α,α-dialkylated residues. α,α-di-n-propylglycine (Dpg) and α,α-di-n-butylglycine (Dbg), have been established by x-ray diffraction. Boc-Ala-Dpg-Alu-OMe (I) and Boc-Ala-Dbg-Ala-OMe (III) adopt distorted type II β-turn conformations with Ala (1) and Dpg/Dbg (2) as the corner residues. In both peptides the conformational angles at the Dxg residue (I: ? = 66.2°, ψ = 19.3°; III: ? = 66.5°. ψ = 21.1°) deviate appreciably from ideal values for the i + 2 residue in a type II β-turn. In both peptides the observed (N…O) distances between the Boc CO and Ala (3) NH groups are far too long (1: 3.44 Å: III: 3.63 Å) for an intramolecular 4 → 1 hydrogen bond. Boc-Ala-Dpg-Ata-NHMe (II) crystallizes with two independent molecules in the asymmetric unit. Both molecules HA and HB adopt consecutive β-turn (type III-III in HA and type III-I in IIB) or incipient 3₁₀-helical structures, stabilized by two intramolecular 4 → 1 hydrogen bonds. In all four molecules the bond angle N-C^α-C′ (τ) at the Dxg residues are ≥ 110°. The observation of conformational angles in the helical region of ?,ψ space at these residues is consistent with theoretical predictions. © 1995 John Wiley & Sons, Inc.     

Conformational difference between diastereomers of Dnp-Val-Aib-Gly-Leu-pNA studied by x-ray crystal analyses

In order to investigate the Conformational change of the α-aminoisobutyric acid (Aib) containing peptide by the D /L replacement of an amino acid residue, single crystals of two diastereomers, Dnp-L -Val-Aib-Gly-L -Leu-pNA (L -L isomer) and Dnp-D -Val-Aib-Gly-L -Leu-pNA (D -L isomer), were prepared from aqueous methanol solutions as CH₃OH and CH₃OH · H₂O solvates, respectively, and were analyzed by the x-ray diffraction method. Molecular conformation of L -L isomer adopts consecutive two different types of β-turns, a type II′ β-turn bent at Aib-Gly, and a type III β-turn bent at Gly-Leu, stabilized by two intramolecular (Leu) NH …? O?C (Val) and (pNA) NH …? O?C(Aib) hydrogen bonds. In contrast, these two intramolecular hydrogen bonds lead the D -L isomer to a distorted 3₁₀-helix conformation consisting of consecutive two type-III β-turn of Aib-Gly-Leu sequence. The most significant structural difference between these diastereomers is the mutual orientation between the Dnp and pNA chromophores. While the extensive stacking of both the chromophores is intramolecularly formed for the folded conformation of L -L isomer, they are oriented toward an opposite direction in the open conformation of D -L isomer and are intermolecularly stacked with each other. The large separation between these diastereomers observed in the chromatography is discussed in the relation with their Conformational differences. © 1993 John Wiley & Sons, Inc.     

Solvent and side-chain contributions to the two-cis ⇄ all-trans equilibria of cyclic hexapeptides,cyclo(Xxx-Pro-D-Yyy)2

Cyclic hexapeptides of the type cyclo(L -Xxx-L -Pro-D -Yyy)₂ or cyclo(L -Xxx-L -Pro-Gly)₂ exist in solution predominantly in two forms of C₂ average symmetry, one with all-trans peptide bonds and generally well-established conformation, and another with both Xxx-Pro peptide bonds cis. We have been measuring the thermodynamic parameters of this equilibrium using carbon and proton nmr spectroscopy. Data have been obtained for peptides in which Yyy = Gly, D -Ala, or D -Phe, and Xxx = Gly, L -Ala, L -Leu, and L -Val. In a given solvent, stability of the all-trans form decreases (ΔG⁰ increases) as Xxx is changed through the series Gly, L -Ala-, L -Leu, and L -Val, consistent with expected increasing repulsion between the Xxx side chain and the proline δ methylene across the trnas Xxx-Pro bond. Also, for a given set of side chains, the stability of the all-trnas form increases as the polarity of the solvent decreases, consistent with models in which all C?O and N? H groups are accessible for solvation in the two-cis form, but two C?O and two N? H groups are somewhat sequestered in the all-trans form. With the available data it is not possible to identify pure intramolecular (solvent-independent) or pure peptide-bond solvation (side chain-independent) terms in ΔH° or ΔS°, although trends are discernible.     

Influence of D and L amino-acid residues on the conformation of peptides in solution: A carbon-13 nuclear magnetic resonance study of cyclo(prolyl-leucyl)

The ¹³C chemical shifts and spin-lattice relaxation times are reported for cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu). The chemical shifts of the D and L leucyl residues in the cyclic peptides differ from each other by 1.8 and 3.6 parts per million for the α and β carbons, respectively. The α-carbons of the prolyl residues differ by 1.0 ppm as a consequence of proximity to a D or an L leucyl residue. The ¹³C spin-lattic relaxation time(T₁) of the prolyl residues, but not the leucyl residues, in both compounds are indicative of difference in conformational equilibria within the pyrrolidine ring in the L -L isomer as compared to the L -D isomer. Anisotropic overall molecular reorientation is not responsible for the differences observed in the T₁ values. The differences in T₁ values and chemical shifts between cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu) appear to result from a difference in conformations of the two diketopiperazine rings.     

Design of Peptides Using α,β-Dehydro-residues: Synthesis,Crystal Structure and Molecular Conformation of N-Boc-L-Val-ΔPhe–ΔPhe-L-Ala-OCH3

To obtain general rules of peptide design using α,β-dehydro-residues, a sequence with two consecutive ΔPhe-residues, Boc-L -Val-ΔPhe–ΔPhe- L -Ala-OCH₃, was synthesized by azlactone method in solution phase. The peptide was crystallized from its solution in an acetone/water mixture (70:30) in space group P6₁ with a=b=14.912(3) Å, c= 25.548(5) Å, V=4912.0(6) ų. The structure was determined by direct methods and refined by a full matrix least-squares procedure to an R value of 0.079 for 2891 observed [I?3σ(I)] reflections. The backbone torsion angles ?₁=?54(1)°, ψ₁= 129(1)°, ω₁=?177(1)°, ?₂ =57(1)°, ψ₂=15(1)°, ω₂ =?170(1)°, ?₃=80(1)°, ψ₃ =7(2)°, ω₃=?177(1)°, ?₄ =?108(1)° and ψ^T₄=?34 (1)° suggest that the peptide adopts a folded conformation with two overlapping β-turns of types II and III′. These turns are stabilized by two intramolecular hydrogen bonds between the CO of the Boc group and the NH of ΔPhe³ and the CO of Val¹ and the NH of Ala⁴. The torsion angles of ΔPhe² and ΔPhe³ side chains are similar and indicate that the two ΔPhe residues are essentially planar. The folded molecules form head-to- tail intermolecular hydrogen bonds giving rise to continuous helical columns which run parallel to the c-axis. This structure established the formation of two β-turns of types II and III′ respectively for sequences containing two consecutive ΔPhe residues at (i+2) and (i+3) positions with a branched β-carbon residue at one end of the tetrapeptide.     

Structurally symmetrical,easily polarizable hydrogen bonds between side chains in proteins and proton-conducting mechanisms. III

(L -Cys)_n, (L -Lys)_n, and (L -Glu)_n were studied by ir spectroscopy in terms of their degree of deprotonation or protonation. It is shown that structurally symmetrical, easily polarizable SH ?S^? ? ^?S ?HS, N⁺H ?N ? N ?H⁺N, and OH ?O^? ? ^?O ?HO hydrogen bonds are formed between the side chains. The different wave number distributions of the ir continua caused by these hydrogen bonds show that the barrier in the double-minimum proton potential decreases in the series of these hydrogen bonds. The stability of these hydrogen bonds against hydration increases in this series. The OH ?O^? ? ^?O ?HO bonds are not broken by small amounts of water. With (L -Cys)_n the formation of easily polarizable hydrogen bonds and a β-structure–coil transition are strongly interdependent. As a result of this coupling effect, the β-structure–coil transition becomes cooperative. With (L -Glu)_n, the formation of the polarizable hydrogen bonds and the observed conformational change are independent processes. The (L -Glu)_n conformation changes from α-helix to coil only if more than 80% of the residues are deprotonated. Finally, on the basis of the various types of easily polarizable hydrogen bonds, charge shifts in active centers of enzymes and the proton-conducting mechanism through hydrophobic regions of biological membranes are discussed.     

Vibrational analysis of peptides,polypeptides, and proteins. XVIII. Conformational sensitivity of the α-helix spectrum: αI- and αII-Poly(L-alanine)

The α_II-helix (? = ?70.47°, ψ = ?35.75°) is a structure having the same n and h as the (standard) α_I-helix (? = ?57.37°, ψ = ?47.49°). Its conformational angles are commonly found in proteins. Using an improved α-helix force field, we have compared the vibrational frequencies of these two structures. Despite the small conformational differences, there are significant predicted differences in frequencies, particularly in the amide A, amide I, and amide II bands, and in the conformation-sensitive region below 900 cm^?1. This analysis indicates that α_II-helices are likely to be present in bacteriorhodopsin [Krimm, S. & Dwivedi, A. M. (1982) Science 216 , 407–408].     

Vibrational CD of polypeptides. X. A study of alpha-helical oligopeptides in solution

We have measured the vibrational CD (VCD) of a series of heterooligopeptides—o-nitrophenylsulfenyl(L -Met-L -Met-L -Leu) _n-OEt, n = 6,8,10,11–in the amide A, I, and II regions. These spectra are identical in shape and magnitude, within our signal to noise limits. The VCD in each band are of exactly the shape expected for a right-handed α-helix and imply that VCD of the polypeptide α-helix is relatively unaffected by chain length down to the 18-subunit level.     

Differential scanning calorimetry studies of NaCl effect on the inverse temperature transition of some elastin-based polytetra-, polypenta-, and polynonapeptides

Differential scanning calorimetry studies of the effect of NaCl on protein-based polymer self-assembly has been carried out on six elastin-based synthetic sequential polypeptides- i.e., the polypentapeptide (L -Val¹-L -Pro²-Gly³-L -Val⁴-Gly⁵)_n and its more hydrophobic analogues (L -Leu¹-L -Pro²-Gly³-L -Val⁴-Gly⁵)_n and (L -Val¹-L -Pro²-L -Ala³-L -Val⁴-Gly⁵)_n; the polytetrapeptide (L -Val¹-L -Pro²-Gly³-Gly⁴)_n and its more hydrophobic analogue (L -IIe¹-L -Pro²-Gly³-Gly⁴)_n; and the polynonapeptide (a pentatetra hybrid), (L -Val¹-L -Pro²-Gly³-L -Val⁴-Gly⁵-L -Val⁶-L -Pro⁷-Gly⁸-Gly⁹)_n. Previous physical characterizations of the polypentapeptides have demonstrated the occurrence of an inverse temperature transition since increase in order of the polypentapeptide, as the temperature is raised from below to above that of the transition, has been repeatedly observed using different physical characterizations. In the present experiments, it is observed that the transition temperatures of the polypeptides studied are linearly dependent on NaCl concentration. The molar effectiveness of NaCl in shifting the transition temperature ΔT_m/[N], is about 14°C/[N], with the dependence on peptide hydrophobicity being fairly small. Interestingly, however, the δΔQ/ [N] does depend on the hydrophobicity of a polypeptide.     

Nuclear magnetic resonance study of ring conformations of cyclic tetradepsipeptide AM-toxins and related peptides

Cyclic tetradepsipeptides, AM-toxin I and II, are the host-specific phytotoxins of Alternaria mali. In order to elucidate conformation-toxicity relationships, we analyzed the 270-MHz proton nmr spectra of AM-toxins and hydrogenated analogs, (D -Ala²)AM-toxin I (toxic) and (L -Ala²)AM-toxin I (not toxic), in (C²H₃)₂SO. These cyclic tetradepsipeptides do not contain N-substituted amino acid residues, and all the peptide and ester groups have been found to be transoid. Two conformers with very unequal populations have been found for AM-toxin I and II; the C^β?C^α? C?O conformations of the Dha² residues are nonplanar S-trans in the major conformer and nonplanar S-cis in the minor conformer. Only one ring conformation has been found for each of (L -Ala²) and (D -Ala²)AM-toxin I. (L -Ala²)AM-toxin I takes a C₄-type ring conformation; all the C?O groups and C^α-H bonds are oriented to the same side of the ring. (D -Ala²)AM-toxin I takes a new ring conformation; the side chain and C?O group of the L -Amp¹ residue are oriented to the same side of the ring. This new conformation is also found for the major conformers of AM-toxin I and II and thus appears to be required for the toxicity. The ring conformations of Tyr(OCH₃)¹-bearing analog tetradepsipeptides have been found to be much the same as those of Amp¹-bearing depsipeptides. Furthermore, on the basis of the two distinct conformations of (D -Ala²) and (L -Ala²)AM-toxin I, an empirical rule is proposed for the stable ring conformations of cyclic tetra-D ,L -peptides, not containing N-substituted amino acid residues.     

A high-resolution 13C-nmr study of collagenlike polypeptides and collagen fibrils in solid state studied by the cross-polarization–magic angle-spinning method. Manifestation of conformation-dependent 13C chemical shifts and application to conformational characterization

We have recorded high-resolution ¹³C-nmr spectra of collagen fibrils in the solid state by the cross-polarization–magic-angle-spinning(CP–MAS)method and analyzed the spectra with reference to those of collagenlike polypeptides. We used two kinds of model polypeptides to obtain reference ¹³C chemical shifts of major amino acid residues of collagen (Gly, Pro, Ala, and Hyp): the 3₁-helical polypeptides [(Gly)_nII, (Pro)_nII, (Hyp)_n, and (Ala? Gly? Gly)_nII], and the triple-helical polypeptides [(Pro? Gly? Pro)_n and (Pro? Ala? Gly)_n]. Examination of the ¹³C chemical shifts of these polypeptides, together with our previous data, showed that the ¹³C chemical shifts of individual amino acid residues are the same, within experimental error (±0.5 ppm), among different polypeptides with different primary sequences, if the conformations are the same. We found that the ¹³C chemical shifts of Ala residues of the 3₁-helical (Ala? Gly? Gly)_n and triple-helical (Pro? Ala? Gly)_n are significantly displaced, compared with those of the α-helix, β-sheet, and silk I form, and can be utilized as excellent probes to examine conformational features of collagen-like polypeptides. Further, the ¹³C chemical shifts of Gly and Pro residues in the triple-helical polypeptides are substantially displaced from those found in (Gly)_nII and (Pro)_nII of the 3₁-helix, reflecting further conformational change from the 3₁-helix to the supercoiled triple helix. In particular, the ¹³C chemical shifts of Gly C ? O carbons of the triple-helical polypeptides are substantially displaced upfield (4.1–5.1 ppm), with respect to those of the 3₁-helical polypeptides. These displacements are interpreted by that Gly C ? O of the former is not involved in NH …? O ? C hydrogen bonds, while this carbon of the latter is linked by these kinds of hydrogen bonds. On the basis of these ¹³C chemical shifts, as reference data for the collagenlike structure, we were able to assign the ¹³C-nmr peaks of Gly, Ala, Pro, and Hyp residues of collagen fibrils, which are in good agreement with the values expected from the model polypeptides mentioned above. We also discuss a plausible conformational change of collagen fibrils during denaturation.     

Conformational studies of heterochiral peptides with diastereoisomeric residues: Crystal and molecular structures of linear dipeptides derived from leucine,isoleucine, and allo-isoleucine

The x-ray diffraction analyses of three N- and C-terminally blocked L , D dipeptides, namely t-Boc-D -Leu-L -Leu-OMe ( 1 ), t-Boc-L -Ile-D -alle-OMe ( 2 ), and t-Boc-D -aIle-L -Ile-OMe (3) containing enantiomeric or diastereomeric amino acid residues have been carried out. The structures were determined by direct methods and refined anisotropically to final R factors of 0.077. 0.058. and 0.072 for ( 1 ) ( 2 ) and ( 3 ), respectively. Peptides 1–3 all assume a similar U-shaped structure with ? and ψ torsion angles cosrresponding to one of the possible calculated minimum energy regions (regions E and G for L residues, and F*. D* and H* for D residues). The peptide backbones of 1-3 are almost super-imposable [provided that the appropriate inversion of the chiral centers of ( 2 ) is made]. Side-chain conformations of Leu residues in peptide ( 1 ) are g^? (tg^?) for the L -Leu residue and the mirrored g⁺ (tg⁺) for the D -Leu residue; however, in peptides ( 2 ) and ( 3 ) the conformations of the isoconfiguralional side chains of the Ile or allo-Ile residues are (g^?t) t and (tg⁺) tfor the L -Ile and the D -allo-Ile moieties, respectively. In all cases, these conformations correspond to the more populated conformers of β-branched residues statistically found in crystal structures of small peptides. The results seem to indicate that, at least in short peptides with enantiomeric or diastereoisomeric residues, the change in chirality in the main-chain atoms perturbs the backbone conformation to a lesser extent and the side chain conformation to a greater extent. © 1995 John Wiley & Sons, Inc.     

Relationship between conformation and physicochemical properties of polypeptides. I. Synthesis of homo- and co-oligopeptides by the liquid-phase method

The synthesis of the following oligo- and co-oligopeptides by the liquid-phase method is described: (L -Met)₁₅ (I), [L -Glu(OBzl)]₂₀ (II), (L -Val)₈-Gly (IV), (L -Ile)₈-Gly (V), (L -Ile)₄-Gly-(L -Ile)₄ (VI), (L -Ile)₄-Pro-(L -Ile)₄ (VII), (L -Met)₅-L -Pro-(L -Met)₅ (VIII), [L -Glu(OBzl)]₇-L -Pro-[L -Glu(OBzl)]₇ (IX). The oligomers are covalently bound to bifunctional polyethylene glycol (PEG) and monofunctional PEG-M of M_r 5 × 10³?2 × 10⁴. Analytical controls were carried out after each step of synthesis in order to ensure quantitative coupling yields. All products could be obtained in high purity as indicated by amino acid analysis, thin-layer chromatography and chiroptical methods. The solubility of the oligomers was strongly enhanced by the presence of the C-terminal PEG group, enabling conformational investigations in a variety of solvents. A significant relationship between conformation and physicochemical properties of the oligopeptides was observed. Oligomers with tendencies to adopt α-helical (I, II) or unordered structures (VI–IX) showed no pronounced change in solubility or coupling kinetics during chain elongation, whereas the onset of a β-structure (IV, V) was paralleled by a drastic decrease in solubility and reactivity of the terminal amino groups. Most notably, the insertion of a proline or glycine in the middle of a β-forming peptide chain (VI, VII) resulted in a considerable increase in solubility compared to the corresponding homo-oligomers. The impact of the conformational properties of a peptide chain on strategic considerations of peptide synthesis in solution is delineated.     

Infrared and Raman study in the solid state of fully protected,monodispersed homooligopeptides of L-valine,L-isoleucine,and L-phenylalanine

An ir-absorption and Raman-scattering study, in the solid state, has been carried out on monodispersed, N- and C-protected homooligopeptides (number of residues, n, from 2 to 7) of L -valine, L -isoleucine, and L -phenylalanine. The amide I, II, III, V, and vNH regions have been examined. Some deuterated (ND) samples have been examined to complete the assignments. L -Phenylalanine dipeptide displays spectral characteristics compatible with the parallel β-structure; L -isoleucine and L -valine dipeptides are probably in a distorted structure. A mixture of parallel and antiparallel extended chains cannot be excluded for the peptides with n = 3. In the amide I region the spectra of peptides with n ≥ 4 show the existence of the β-conformation. The problem of chain orientation within the pleated-sheet structure is discussed on the basis of a recent theoretical treatment of vibrational interactions of the amide I mode.     

Proton transfer and polarizability of hydrogen bonds formed between cysteine and lysine residues

(L -Cys)_n + N-base systems and (L -Cys)_n + (L -Lys)_n systems were studied by ir spectroscopy. It is shown that in the water-free systems, SH ?N ? S^? ?H⁺N hydrogen bonds are formed. With the (L -Cys)_n + N-base systems, both proton-limiting structures in the SH ?N ? S^? ?H⁺N bonds have equal weight when the pK_a of the protonated N-base is 2 pK_a units larger than that of (L -Cys)_n. The same is true with the water-free (L -Cys)_n + (L -Lys)_n system. Thus, with regard to the type of proton potentials present, these hydrogen bonds are proton-transfer hydrogen bonds showing very large proton polarizabilities. This is confirmed by the occurrence of continua in the ir spectra. Small amounts of water open these hydrogen bonds and increase the transfer of the proton to (L -Lys)_n. In the (L -Lys)_n + N-base systems, with increasing proton transfer the backbone of (L -Cys)_n changes from antiparallel β-structure to coil. In (L -Cys)_n + (L -Lys)_n, the conformation is determined by the (L -Lys)_n conformation and changes depending on the chain length of (L -Lys)_n. Finally, the reactivity increase in the active center of fatty acid synthetase, which should be caused by the shift of a proton, is discussed on the basis of the great proton polarizability of the cysteine–lysine hydrogen bonds.     

Type II β-turn conformation of pivaloyl-L-prolyl-α-aminoisobutyryl-N-methylamide: Theoretical,spectroscopic, and X-ray studies

Pivaloyl-L -Pro-Aib-N-methylamide has been shown to possess one intramolecular hydrogen bond in (CD₃)₂SO solution, by ¹H-nmr methods, suggesting the existence of β-turns, with Pro-Aib as the corner residues. Theoretical conformational analysis suggests that Type II β-turn conformations are about 2 kcal mol^?1 more stable than Type III structures. A crystallographic study has established the Type II β-turn in the solid state. The molecule crystallizes in the space group P2₁ with a = 5.865 Å, b = 11.421 Å, c = 12.966 Å, β = 97.55°, and Z = 2. The structure has been refined to a final R value of 0.061. The Type II β-turn conformation is stabilized by an intramolecular 4 → 1 hydrogen bond between the methylamide NH and the pivaloyl CO group. The conformational angles are ?_Pro = ?57.8°, ψ_Pro = 139.3°, ?_Aib = 61.4°, and ψ_Aib = 25.1°. The Type II β-turn conformation for Pro-Aib in this peptide is compared with the Type III structures observed for the same segment in larger peptides.     

Crystal state conformation of three model monomer units for the β-bend ribbon structure

The molecular and crystal structures of three compounds, representing the repeating units of the β-bend ribbon (an approximate 3₁₀-helix, with an intramolecular hydrogen-bonding donor every two residues), have been determined by x-ray diffraction. They are Boc-Aib-Hib-NHBzl, Z-Aib-Hib-NHBzl, and Z-L -Hyp-Aib-NHMe (Aib, α-aminoisobutyric acid; Bzl, benzyl; Boc, t-butyloxycarbonyl; Hyp, hydroxyproline Hib, α-hydroxyisobutyric acid; Z, benzyloxycarbonyl). The two former compounds are folded in a β-bend conformation: type III (III′) for Boc-Aib-Hib-NHBzl, while type II (II′) for the Z analogue. Conversely, the structure of Z-L -Hyp-Aib-NHMe, although not far from a type II β-bend, is partially open.