Fourth polymorph of [Phe 4 Val 6] antamanide (pentahydrate)

The cyclic decapeptide antamanide and the synthetic, biologically active analog [Phe⁴ Val⁶] antamanide (cyclic[ValProProPhePhe]₂) crystallize in various crystal forms as a function of the solvent. The present crystalline polymorph obtained from acetone/water (also from ethanol/water and DMSO/water) crystallizes in space group P2₁2₁2₁ with a = 20.194 (30) Å, b = 21.118 (31) Å, c = 16.132 (25) Å and four molecules of peptide in the unit cell. There are five cocrystallized water molecules per peptide molecule, of which four water molecules are intrinsic to the peptide molecule. Although the molecular packing is entirely different in each of the polymorphs, the conformation of the peptide molecule, including the intrinsic water molecules, is very similar in all the polymorphs.     

Water structure in [Phe4 Val6] antamanide • 12H2O crystallized from dioxane

Crystals of [Phe⁴ Val⁶] antamanide (cyclic[ValProProPhePhe]₂) grown from dioxane/H₂O, with space group P2₁2₁2 and cell parameters a= 15.099(4), b = 22.008(5) and c = 11.024(3) Å, are almost identical to crystals grown from H₂O/acetone, the structure of which was determined a number of years ago. Perpeptide molecule there are the equivalent of 12 water molecules occupying 16 sites in both crystals; however, in the new investigation a number of water molecules present at one-half occupancy have been found in different positions than in the earlier analysis. The interpretation of the hydrogen bonding between peptide/water and between water/water is much more satisfactory. Pentagonal water assemblies are present in the solvent channel. There is a distinct indication of the occurrence of a bifurcated bond between two water molecules, as well as the presence of three-center hydrogen bonds joining three water molecules. This may be the first experimental example of a bifurcated bond between two water molecules.     

Ion-binding and pharmacological properties of Tyr6 and Tyr9 antamanide analogs

Abstract: In order to investigate the antiproliferative properties of antamanide, we have synthesized and studied two antamanide analogs where the phenylalanine residue in positions 6 or 9 is substituted by tyrosine, their corresponding linear forms and the cyclic and linear des Phe⁵,Phe⁶–Tyr⁹–analogs. Antamanide and its biologically active synthetic analogs are able to form highly stable complexes with metal ions, particularly Na⁺, K⁺ and Ca²⁺. We studied the ion-binding properties of the Tyr–antamanide analogs by CD and Tb³⁺-mediated fluorescence in acetonitrile. In this medium the far-and near-UV CD spectra of the neat Tyr⁶–antamanide analog are very similar to that of the parent cyclic decapeptide. Substantial differences occur on the contrary in the CD spectra of the neat Tyr⁹–antamanide, particularly in the regions at 220 nm and 270–290 nm. In acetonitrile, as already found for antamanide, the interaction with the above-mentioned metal ions always produces evident changes in the far- and near-UV CD spectra of both analogs. On the contrary, the CD spectra of the linear deca- and octa- and of the cyclic octa-analogs are affected by the presence of metal ions only in the near-UV region. In the same solvent the Tb³⁺-mediated fluorescence spectra of all the synthetic peptides are remarkably affected by the addition of ions. On the basis of the spectral total changes, by using either or both the spectroscopic techniques, it has been possible to determine the ion binding constants for all the linear and cyclic Tyr–antamanide analogs and to compare them with that of the parent peptide. The antitoxic and antiproliferative activities of these antamanide analogs have been tentatively correlated to their ion-binding properties. A preliminary account of this work was given in ( 1 ).     

New patterns of hydrogen bonded interactions between polypeptide chains

Crystals of glycylglycylglycine (C₆H₁₁N₃O₄), grown from an aqueous methanol solution, are triclinic, space group P1, with the unit cell dimensions (at 22 ± 3°) a= 11.656(3), b= 14.817(3), c= 4.823(2) Å, α= 88.45(3), β= 95.96(3), γ= 105.42(3)°, Z = 4 (with two molecules in the asymmetric unit) with a density of D_obs= 1.58g·cm^-3 and D_calc= 1.572g·cm^-3. The crystal structure was solved by a combination of multisolution and trial and error methods and refined with full-matrix least-squares method to a final R value of 0.036 for the observed 3021 reflections (I ≥ 2s?). The conformation of the two molecules I and II in the asymmetric unit is very similar (except around the N-terminal end); they have the fully extended trans-planar conformation, and have ω values ranging from 2 to 4°. The peptide chain repeating distances (C¹_α - C³_α) are 7.27 Å and 7.18 Å in the two molecules as compared with the value of 6.68 Å for extended β-sheets with β-carbons. There are four different interactions between these two molecules characterized by different hydrogen bonding. Molecule I is hydrogen bonded to a neighboring molecule I using four hydrogen bonds. Molecule II is hydrogen bonded to another II, using bifurcated interactions involving the peptide nitrogen. Molecule I is hydrogen bonded to two different molecules II forming distinctly different hydrogen bonding patterns from the two mentioned above. The molecules are packed in rows, in a head-to-tail fashion (C-terminal opposite N-terminal) and are held together in sheets by hydrogen bonds between carbonyl and amide groups, corresponding to the very familiar anti-parallel pleated sheet arrangement for polypeptides. The hydrogen bonds involving the amino nitrogens as donors are significantly longer and presumably weaker compared to those involving the NH⁺₃ group. The C=O distances show variations that correlated with hydrogen bonding. The N-H … O angle varies from 152 to 174° and the bent N-H … O hydrogen bonds show bifurcated interactions.     

Cystine peptides Antiparallel β-sheet conformation of the cyclic biscystine pep tide [Boc-Cys-Ala-Cys-NHCH3]2

The crystal structure analysis of the cyclic biscystine peptide [Boc-Cys¹-Ala²-Cys³-NHCH₃]₂ with two disulfide bridges confirms the antiparallel β-sheet conformation for the molecule as proposed for the conformation in solution. The molecule has exact twofold rotation symmetry. The 22-membered ring contains two transannular NH ? OC hydrogen bonds and two additional NH ? OC bonds are formed at both ends of the molecule between the terminal (CH₃)₃COCO and NHCH₃ groups. The antiparallel peptide strands are distorted from a regularly pleated sheet, caused mainly by the L-Ala residue in which φ=– 155° and ψ= 162°. In the disulfide bridge C^α (1)-C^β (1)-S(1)-(3′)-C^β(3′)-C^α(3′), S—S = 2.030 Å, angles C^β SS = 107° and 105°, and the torsional angles are –49, –104, +99, –81, –61°, respectively. The biscystine peptide crystallizes in space group C2 with a = 14.555(2) Å, b = 10.854(2) Å, c = 16.512(2)Å, and β= 101.34(1) with one-half formula unit of C₃₀H₅₂N₈O₁₀S₄· 2(CH₃)₂SO per asymmetric unit. Least-squares refinement of 1375 reflections observed with |F| > 3σ(F) yielded an R factor of 7.2%.     

Conformational investigation of α, β-dehydropeptides

The crystal structure of Ac-Pro-ΔVal-NHCH₃ was examined to determine the influence of the α,β-dehydrovaline residue on the nature of peptide conformation. The peptide crystallizes from methanol-diethyl ether solution at 4° in needle-shaped form in orthorhombic space group P2₁2₁2₁ with a= 11.384(2) Å, b = 13.277(2) Å, c = 9.942(1) Å. V = 1502.7(4) ų Z = 4, D_m= 1.17 g cm^?3 and D_c=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 β-bend between the type I and the type III conformation with φ₁=?68.3(4)°, ψ₁=? 20.1(4)°, φ₂=?73.5(4)°= and Ψ₂=?14.1(4)°=. An intramolecular hydrogen bond between the carbonyl oxygen of ith residue and the NH of (i+ 3)th residue stabilizes the β-bend. An additional intermolecular N.,.O hydrogen bond joins molecules into infinite chains. In the literature described crystal structures of peptides having a single α,β-dehydroamino acid residue in the (i+ 2) position and forming a β-bend reveal a type II conformation.     

Crystal structure of L-lysyl-L-glutamic acid dihydrate

L-Lysyl-L-glutamic acid dihydrate, C₁₁N₃O₅H₂₁·2H₂O, crystallizes in the monoclinic space group P2₁ with a = 12.474(2), b = 5.020(1), c = 13.157(2) Å, β= 114.69(1)° and Z = 2. The crystal structure was solved by direct methods and refined to an R value of 0.037 using full matrix least-squares method. The molecule exists as a double zwitterion with both the amino and carboxyl groups ionised. The peptide has a folded conformation with its Lys residue trans and Glu residue gauche^?gauche⁺. The side chains of the Lys and Glu residues correspond to all trans and folded (g^?g^?g^?) conformations respectively. The terminal carboxyl group forms hydrogen bonds with the ξ-amino group of the lysine side chain. The head-to-tail interaction often seen in peptide crystals is absent in the present structure. In the extended crystal structure water molecules form channels along the b direction and are enclosed within helically arranged hydrogen bonds formed by the lysine side chain and the peptide backbone.     

Backbone—side-chain interactions in serine Synthesis,crystal structure and solution conformation of a linear model peptide N-Boc-l-Ser-l-Phe-OCH3

The peptide Boc-Ser-Phe-OCH₃ was synthesised by a solution-phase method using the usual workup procedure. The peptide was crystallized from a 70:30 (v/v) methanol-water mixture. The crystals are monoclinic, space group P2₁ with a= 5.128(2), b=17.873(2), c=11.386(2) Å, and β=98.03(3)°. The structure was determined by direct methods and refined by a structure factor least-squares procedure. The final R-value for 1499 observed reflections was 0.041. The structure contains one peptide and one solvent water molecule. The peptide adopts a β-strand-like conformation with φ₁=- 100.3(5), ψ_l= 99.9(5), φ₂= - 122.2(5), ψ^T₂= -172.5(6)°. The Ser side-chain assumes an extended conformation with χ¹₁= - 177.0(4)°. The O^γH group of serine acts as a proton donor in an intramolecular weak hydrogen bond with (Ser) O′₁; [O^γ₁;-H^γ₁?O′₁= 3.253(6) Å]. The Phe side-chain adopts a staggered conformation with χ¹₂= -70.9(6), χ²_2,1= 88.4(7)°, χ^2,2₂= -89.2(6)°. The water molecule generates a loop through two hydrogen bonds with O^γ₁ [OW?O^γ₁= 2.893(5) Å] and O′₂ [OW-O′₂= 2.962(7) Å] atoms. The unit-translated peptide molecules along the α-axis are held by hydrogen bonds: N₁-H₁?O₂ (x-1, y, z) = 2.954(4) Å and N₂-H₂?O′₁ (x+1, y, z) = 2.897(6) Å in a manner similar to those observed in parallel β-pleated sheet structures. There is an additional interaction involving O^γ₁ and the water molecule [OW?O^γ₁ (x= 1, y, z) = 2.789(4) Å]. The strong NOE peak of C_i(H)?N_i+1 (H) and a simultaneous weak NOE peak of N_i(H)?N_i+l (H) in the ROESY spectra of two-dimensional NMR in dimethyl sulfoxide indicate a β-strand-like conformation for the peptide in solution. © Munksgaard 1996.     

Crystal structure and conformation of polypeptides: L-leucylglycylglycylglycine

Crystals of L-leucylglycylglycylglycine, LGGG (C₁₂H₂₂N₄O₅), grown from an ethanol-water solution, are orthorhombic, space groups P2₁2₁2₁, with unit cell dimensions (at 22 ± 3°) a = 9.337(1), b = 10.995(1), c = 15.235(1)Å, v = 1563.4 ų, Z = 4 with a density of D_obs= 1.29 g-cm^-3 and D_calc= 1.279 g°cm^-3. The crystal structure was solved by the application of direct methods and refined to an R value of 0.029 for 1018 reflections with I ± 2s?. The molecule exists as a zwitterion in the crystal. The trans peptide backbone takes up a folded conformation at the middle glycylglycyl link accompanied by a significant nonplanarity up to Δω of 8° at the middle peptide and is relatively more extended at the two ends. The molecules are linked together intermolecularly in an infinite sequence of head to tail 1–4′ hydrogen bonds, as is typical of charged peptides. It is interesting to note that while glycylglycylglycine takes up an extended β-sheet conformation, addition of Leu to the N-terminal results in a bent conformation.     

Structural characteristics of diproline: a new crystal form of tBoc-Pro-Pro-OH

The structure of a new crystalline form of tBoc-Pro-Pro-OH (C₁₅ H₂₄ N₂ O₅) has been determined. The crystals were monoclinic, P2₁ a = 14.667(5), b = 16.600(4), c = 15.502(3) Å, β= 117.84(2)?, V= 3337.2 ų and Z= 8, D_c= 1.24g/cm³. There are four molecules in the asymmetric unit, each displaying polyproline-type structure but differing in the proline pucker. All four molecules display a twist conformation in the first proline ring, with molecules A, B and C being ^β_γT (P ～ 183?, τ 33 for A and B, t～18 for C) and molecule D between ^β_γT and _γE (P= 10°, τ38). The second residue of all four molecules has an envelope conformation. Molecules A and B display an ^αE conformation (P～126?, t～25) and molecules C and D display a ^βE conformation (P～168?, τ37). The molecules are hydrogen-bonded (O…OH), forming helical channels along the a-axis.     

Crystal and molecular structure of Boc-Phe-Val-OMe; comparison of the peptide conformation with its dehydro analogue

The crystal structure of the peptide Boc-Phe-Val-OMe determined by X-ray diffraction methods is reported in this paper. The crystals grown from aqueous methanol are orthorhombic, space group P 2₁2₁ 2₁, a= 11.843(2), b= 21.493(4), c= 26.676(4) A and V= 6790 ų. Data were collected on a CAD4 diffractometer using MoK_α radiation (λ= 0.7107 Å) up to Bragg angle θ=26°. The structure was solved by direct methods and refined by a least-squares procedure to an R value of 6.8% for 3288 observed reflections. There are three crystal-lographically independent peptide molecules in the asymmetric unit. All the three molecules exhibit extended conformation. The sidechain of the Val² residue shows two different conformations. The conformation of the peptide Boc-Phe-Val-OMe is compared with the conformation of Ac-ΔPhe-Val-OH. It is observed that while Boc-Phe-Val-OMe exhibits an extended conformation, Ac-ΔPhe-Val-OH shows a folded conformation. The results of this comparison highlight the conformation constraining property of the ΔPhe residue. Interestingly, even though Boc-Phe-Val-OMe and Ac-ΔPhe-Val-OH are conformation ally different, they exhibit similar packing patterns in the solid state. © Munksgaard 1995.     

Crystal structure of Boc-LAla-ΔPhe-ΔPhe-ΔPhe-ΔPhe-NHMe: a left-handed helical peptide

αβ-Dehydrophenylalanine residues constrain the peptide backbone to β-bend conformation. A pentapeptide containing four consecutive (APhe) residues has been synthesised and crystallised. The peptide Boc-LAla-ΔPhe-ΔPhe-ΔPhe-ΔPhe-NHMe (C₄₅H₄₆N₆O₇, MW = 782.86) was crystallised from an acetonitrile/ methanol mixture. The crystal belongs to the orthorhombic space group P2₁2₁2₁ with a = 19.455(6), b = 20.912(9), c = 11.455(4) Å and Z = 4. The X-ray (MoK_α, lD = 0.7107 Å) intensity data were collected using the Rigaku-AFC7 diffractrometer. The crystal structure was determined by direct methods and refined using the least-squares technique, R = 8.41% for 1827 reflections with ‖F₀‖ > 4σ‖F_o‖. The molecule contains the largest stretch of consecutive dehydrophenylalanine residues whose crystal structure has been determined so far. The peptide adopts left-handed 3₁₀-helical conformation despite the presence of LAla at the N-terminus. The mean ø, Ψ values, averaged across the last four residues are 56.8° and 17.5°, respectively. There are four 41 intramolecular hydrogen bonds, characteristic of the 3₁₀-helix. In the crystal each molecule interacts with four crystallographically symmetric molecules with one hydrogen bond each.     

Synthesis and properties of chemotactic peptide analogs

As a part of a research program aimed at studying structure activity relationship in the field of chemotactic peptides, modified analogs of the potent chemoattractant HCO-Met-Leu-Phe-OH (fMLP) of the general formula HCO-Xaa-Leu-Yaa-OMe are examined. 4-Aminotetrahydrothiopyran-4-carboxylic acid (Thp) and 2-aminoindane-2-carboxylic acid (Ain) have been chosen as achiral, conformationally restricted amino acids suitable to mimick the external Met and Phe residues of fMLP-OMe. Studies on a first model, namely [Ain³]fMLP-OMe 1, have already been reported (12). Here the two remaining analogs (Thp¹, Ain³) 2 and [Thp¹] 3 have been synthesized. The conformation in the crystal of the disubstituted analog 2 has been determined and compared with those adopted by the parent fMLP-OMe and by previously studied models. The backbone conformation of 2 is characterized by helical folding centred at each of the three residues with the central Leu presenting helical handedness opposite to those of the two adjacent achiral residues. This conformation presents strong similarities with that adopted in the crystal by fMLP-OMe and resembles the conformation of fMLP bound to immunoglobulin (Bence-Jones dimer). The conformationally restricted analogs 2 and 3 are more active than the parent in the stimulation of directed mobility of human neutrophils but are practically inactive in the superoxide production. Crystals of 2 are orthorhombic, s.g. P 2₁ 2₁ 2₁, with a = 21.934 (8), b = 10.856 (2), c = 10.380 (2) Å. The structure has been refined to R = 0.071 for 2301 independent reflections with I > 1.5 σ.     

Synthesis,crystal structure and molecular conformation of the tBuCO-D,L-Ala-Δz-Phe-NhiPr α,β-unsaturated dipeptide

The crystal structure of the tBuCO-d,l -Ala-Δ^z-Phe-NHiPr dipeptide has been solved by X-ray diffraction. The peptide crystallizes in monoclinic space group P2JC with a = 13.445 (3) Å, b = 35.088 (4) Å, c = 14.755(3) Å, β= 116.73(1)°, Z = 12 and d_c= 1.151 g.cm^?3. The three independent molecules per asymmetric unit accommodate a βII-folded conformation, but only one of them contains the typical i + 3 → i interaction characterizing a β-turn. In the other two molecules, the N…O distance exceeds 3.2 Å, a value generally considered the upper limit for hydrogen bonds in peptides. In solution, the βII-turn conformation is largely predominant.     

Crystal structure of deltakephalin: a γ-selective opioid peptide with a novel β-bend-like conformation

The solid-state structure of deltakephalin (Tyr-D Thr-Gly-Phc-Leu-Thr) has been determined by single-crystal X-ray diffraction. Deltakephalin (DTLET) is a synthetic opioid peptide which differs from enkephalin in that a d -Thr has been substituted for Gly² and a sixth residue, l -Thr, has been added. Clear colorless plates obtained using vapor diffusion and macro-seeding crystallization techniques were monoclinic; space group C2 with u = 27.389(5), b = 9.205(2), c = 16.788(2) Å, β= 98.87(2) ˚ and V= 4181.4(14) ų. The asymmetric unit contained one molecule of DTLET and six molecules of water, giving a calculated density of 1.28 g cm⁻³. The crystal structure revealed that DTLET has a pseudo type I'β-bend which is stabilized by an intramolecular side-chain to backbone hydrogen bond. This is the first reported observation of a pseudo β-bend conformation in a solid-sate structure of an enkephalin analog.     

Crystal structure of a dipeptide Boc-Aib-Phe-OMe

In order to understand the effect of the restrictions posed by the Aib residue on peptide conformation we studied the crystal structure of a dipeptide tBoc-Aib-Phe-OMe. Crystals of this compound are triclinic, space group PI with a= 9.600(1) Å, b=10.262(1) Å, c= 10.799(1) Å, α= 98.43°(1), β=99.18°(1), °=98.87°(1), V= 1021.69(18) ų and Z=2. The structure was solved by direct methods and refined to an R-factor of 4.98%. The backbone conformational angles for the Aib residue in molecule A are in the left-handed helical region, while in molecule B they are in the right-handed helical region. The Phe residue in molecule A is in the right-handed helical conformation, while in molecule B it is in the β-region. The peptide units are trans and show significant deviation from planarity [(ω₁= 166.67(5)° and ω₂=–177.9(5)]. © Munksgaard 1997.     

Synthesis and crystal structures of Boc-L-Asn-L-Pro-OBzl·CH3OH and dehydration side product,Boc-β-cyano-L-alanine-L-Pro-OBzl

Boc-L-Asn-L-Pro-OBzl:C₂₁H₂₉O₆N₃·CH³OH, M_r= 419.48 + CH₃OH, monoclinic, P2₁, a= 10.049(1), b= 10.399(2), c= 11.702(1)Åβ= 92.50(1)°, V = 1221.7(3)ų, d_x= 1.14g cm^-3, Z = 2, CuKα (λ= 1.54178 Å), F(000) = 484 (with solvent), 23°, unique reflections (I > 3σ(I)) = 1745, R = 0.043, R_w= 0.062, S = 1.66. Boc-β-cyano-L-alanine-L-Pro-OBzl: C₂₁H₂₇O₅N₃, M_r= 401.46, orthorhombic, P2₁2₁2₁, a= 15.741(3), b= 21.060(3), c= 6.496(3)ÅV= 2153(1)ų, d_x= 1.24g·cm^-3, Z = 4, CuKα (λ= 1.54178 Å), F(000) = 856, 23°, unique reflections (I > 3σ(I)) = 1573, R = 0.055, R_w= 0.078, S = 1.86. The tert.-butyloxycarbonyl (Boc) protected dipeptide benzyl ester (OBzl), BOC-L-Asn-L-Pro-OBzl, prepared from a mixed anhydride reaction using isobutylchloroformate, BOC-L-asparagine, and HCI·L-proline-OBzl, crystallized with one methanol per asymmetric unit in an extended conformation with the Asn-Pro peptide bond trans. Intermolecular hydrogen bonding occurs between the methanol and the Asn side chain and between the peptide backbone and the Asn side chain. A minor impurity due to the dehydration of the Asn side chain to a β-CNaia crystallized with a similar extended conformation and a single intermolecular hydrogen bond.     

Heterochiral N-formyl methionyl peptides

Crystal and molecular structures for the heterochiral sequence N-formyl-l -methionine-d -phenylalanine, 1, and its tertiary butyl ester, 2, are reported. The solid-state peptide conformation is compared to that observed in solution by n.m.r. techniques. For N-f-Met-d -Phe, 1, the crystal was orthorhombic, space group P2₁ 2₁2₁ with a cell of dimensions a = 5.061(3), b = 16.575(5) and c = 19.656(6) Å at ambient temperature of 293K; V = 1649(2)ų, Z = 4, D_m= 1.31(2)gcm^?3, D_x= 1.307gcm^?3, μ(Mokx) = 2.047cm^?1. For N-f-Met-d -Phe-OtBu. 2, the crystal was monoclinic, space group P2₁ with a cell of dimensions a = 9.963(2), b = 11.147(2), c = 19.166(3)Å. β= 102.31(1) at 273K; V = 2080(2) ų Z = 4, D_m= 1.22(2)gcm^?3, D_x= 1.215gcm^?3μ(MoKx) = 1.714cm^?1. The structures were solved from diffractometer data and refined to conventional final R = 0.046, R_w= 0.053 for F-Met-d -Phe (1301 observations. I ≥ 3σ(I)) and to R = 0.056, R_w= 0.064 for the t-butylester (2411 observations. I ≥ 3σ(I)). The l-d acid, 1, crystallizes in an extended β-sheet conformation with trans-planar peptide bond; the principal torsion angle values are φ₁=– 141.2(4).Ψ₁= 149.6(4)³, φ₂= 157.4(4)°. The methionine side chain adopts a common coiled conformation with x¹₁= - 58.0(5).x²¹= 175.1(4), x³₁= 76.5(5). The Phe side chain adopts the statistically least favored g orientation in contrast to the most populated rotamer in solution. The crystal structure is composed of parallel β-sheets held together by four weak intermolecular contacts including two C-H O contacts from the alpha carbons to the formyl and peptide carbonyl oxygens. Sheet layers are joined in a head-to-tail fashion through a very short (2.569(4) Å) contact between the carboxyl OH and the formyl oxygen and may be further stabilized by a C-H—O interaction between the formyl proton and the carboxyl OH. Two crystallographically independent molecules are observed in the crystal structure of N-f-l -Met-d -Phe-OtBu, 2. These are distinct conformational isomers differing principally at both the N and C termini. Particularly noteworthy is the synplanar orientation of the ester C = O with respect to the peptide nitrogen in molecule A. which contrasts to the antiplanar orientation in molecule B. Additionally, the formyl group is coiled more towards the C-terminus in molecule B. Principal torsion angles are φ₁(A) = - 120.6(5), Ψ₁(A) = 102.0(6)°, φ₂(A) = 128.1(6), φ₁(B) = - 94.6(5), Ψ₁(B) = 91.9(6)°. 121.7(6)°. The peptide bond is trans-planar in both molecules. Side chain dispositions are essentially identical in both structures. The Met side chain adopts the zig-zag trans-planar conformation while the Phe residue adopts an orientation near + 60° in agreement with rotamer populations observed by solution n.m.r. Typical peptide intermolecular H-bonding is observed in the ester crystal structure; both the peptide and formyl groups participate in the proposed H-bonding scheme.     

Structure and conformation of linear peptides VII.

The tripeptide, L-valyl-glycyl-glycine (C₉H₁₇N₃O₄, molecular weight = 231), crystallizes in the monoclinic space group C2, with a = 24.058(3)Å, b = 4.801(1), c = 10.623(2), β = 110.02(1)° and Z = 4. The structure was determined by direct methods and refined to a final R-index of 0.043 for 830 reflections (sinθ/Λ ≤ 0.53 A^-1) with I> 1.0s?. The molecule exists as a zwitterion. The peptide units are trans and one of them shows significant deviations from planarity (Δω₂ = 9.3°). The peptide chain repeat distance, 1C^α-3Cα, is 7.23Å and the molecule displays a highly extended conformation with backbone torsion angles of ψ₁ = 123.1°, ω₁ = - 179.4°, ø₂ = - 155.1°, ψ;₂ = 154.7°, ω₂ = 170.7°, ø₃ = - 146.6° and ψ₃ = 180.0°. For the valyl side chain, χ₁₁ = - 52.5°, χ₁₂ = 174.2°. The packing involves hydrogen-bonded interactions between successive molecules related by the β-translation of the lattice, giving rise to the familiar parallel β-sheet structure which appears to be the most extended one observed to date.     

Crystal and molecular structure of L-lysyl-L-valine hydrochloride – a new lysine conformation

Thin plates of L-lysyl-L-valine hydrochloride (C₁₁H₂₄N₃O₃Cl) were obtained using the vapour diffusion technique and analysed by X-ray diffraction. The unit cell is orthorhombic, space group P2₁2₁2₁, a = 5.465(6)Å, b = 19.657(4) Å, c = 13.522(2) Å, V = 1452.6(2.1) ų and Z = 4. The structure was solved by direct methods and refined to an agreement factor of 6.7% for 939 reflections with I > 3 σ(I). The lysine side chain conformation (g^- g^- tt) has never been found in peptide crystal structures, although it has been reported to occur in proteins. A network of hydrogen bonds between peptide molecules spreads along the a and c directions while no direct bonds are observed to occur between peptides along the b axis direction. This asymmetric pattern of interactions correlates with the crystal morphology.