X-ray crystal structure of galabiose, O-alpha-D-galactopyranosyl-(1---4)-D-galactopyranose

O-alpha-D-Galactopyranosyl-(1---4)-D-galactopyranose, C12H22O11, Mr = 342.30, crystallises in the orthorhombic space group P2(1)2(1)2(1), and has alpha = 5.826(1), b = 13.904(3), c = 17.772(4) A, Z = 4, and Dx = 1.579 g.cm-3. Intensity data were collected with a CAD4 diffractometer. The structure was solved by direct methods and refined to R = 0.063 and Rw = 0.084 for 2758 independent reflections. The glycosidic linkage is of the type 1-axial-4-axial with torsion angles phi O-5' (O-5'-C-1'-O-1'-C-4) = 98.1(2) degrees, psi C-3 (C-3-C-4-O-1'-C-1') = -81.9(3) degrees, phi H (H-1'-C-1'-O-1'-C-4) = -18 degrees, and psi H (H-4-C-4-O-1'-C-1') = 35 degrees. The conformation is stabilised by an O-3 . . . O-5' intramolecular hydrogen-bond with length 2.787(3) A and O-3-H . . . O-5' = 162 degrees. The glycosidic linkage causes a folding of the molecule with an angle of 117 degrees between the least-square planes through the pyranosidic rings. The crystal investigated contained 56(1)% of alpha- and 44(1)% of beta-galabiose as well as approximately 70% of the gauche-trans and approximately 30% of the trans-gauche conformers about the exocyclic C-5'-C-6' and C-5-C-6 bonds. The crystal packing is governed by hydrogen bonding that engages all oxygen atoms except the intramolecular acceptor O-5' and the glycosidic O-1' oxygen atoms.     

Conformational analysis of levanbiose by molecular mechanics.

A relaxed conformational energy map for levanbiose, O-beta-D-fructofuranosyl-(2----6)-beta-D-fructofuranoside, was computed with the molecular mechanics program MM2(87). All torsion angles of the three linkage bonds were driven by 30 degrees increments while two primary alcohol groups were held at three staggered forms. The steric energy of all other parameters was optimized. The side groups were retained at the same relative positions on the two rings in this first part of the study so our results are directly applicable to the study of polymeric levan with identical repeating units. The low-energy dimers did not lead to viable polymers. The interresidue linkage torsion angles defined by C-6-O-2'-C-2'-C-1' (phi) and O-5-C-5-C-6-O-2' (omega) have minima at +60 degrees and -60 degrees, respectively, with accessible minima at other staggered forms. As observed in inulobiose, the preferred torsion angle at central linkage bond defined by C-5-C-6-O-2'-C-2' (psi) was antiperiplanar. An analysis of all conformations of staggered side groups showed that the C-1 and C-1' groups had little effect but the C-6' group showed a preference for chi-6'(O-5'-C-5'-C-6'-O-6') = -60 degrees. The fructofuranose rings were started at the low-energy 4(3)T conformation (angle of pseudorotation, phi 2 = 265 degrees) that was retained except when the linkage conformations created severe inter-residue conflict.     

Crystal and molecular structure of methyl O-alpha-D-manno-pyranosyl-(1----2)-alpha-D-mannopyranoside

The crystal and molecular structure of a synthetic mannosyl disaccharide, methyl O-alpha-D-mannopyranosyl-(1----2)-alpha-D-mannopyranoside, has been determined from X-ray diffractometer data by direct methods by use of the Multan programs. The crystals are monoclinic, space group P2 with unit cell dimensions, a 8.086(1), b 9.775(1), c 9.975(2) A, beta 104.58(1) degrees, Z 2, and Dm 1.54 g/cm3. The structure was refined to an R-value of 0.033 for 1359 reflections measured with CuK alpha radiation. The mannopyranose units have the chair conformations 4C(D) with C-5' and C-2' deviating from the best plane through the other four atoms of the ring by -0.68 and +0.53 A in the nonreducing group, and C-3 and O-5 deviating from the mean plane through the other four atoms by +0.57 and -0.66 A, respectively, in the "potentially" reducing residue. The ring-to-ring conformation can be described as (phi, psi) = (-64.5, 105.5 degrees). The conformation across the C-5--C-6 bond is gauche-gauche in both the sugars. The crystal structure is stabilized by a network of intermolecular O-H...O hydrogen bonds.     

Energy-minimized conformation of gramicidin-like channels. I. Infinitely long poly-(L,D)-alanine beta 6.3-helix.

The energy-minimized conformation of an infinitely long poly-(L,D)-alanine in single-stranded beta 6.3-helix was calculated by the molecular mechanics method. When energy minimization was started from a wide range of initial geometries, six optimized conformations were obtained and identified as the right- and left-handed counterparts of the beta 4.5-, beta 6.3-, and beta 8.2-helices. It was found that their conformation energies increase in this order, the beta 4.5-helix having the lowest energy. The backbone dihedral angles of the energy-minimized beta 6.3-helix were: phi L = -116 degrees (or -131 degrees), psi L = 122 degrees (or 111 degrees), phi D = 131 degrees (or 116 degrees), psi D = -111 degrees (or -122 degrees), omega L = 173 degrees (or 173 degrees), and omega D = -173 degrees (or -173 degrees) for the right-handed (or left-handed) helix. This helix was composed of 6.30 residues/turn with a pitch of 4.97 A. All the alpha-carbons of L- and D-configurations appeared on one common circular helix. Interestingly, small deviations (approximately 7 degrees) of the peptide bonds from the planar structure caused a considerable lowering of the conformation energy, and, at the same time, they produced more favorable fitting of the hydrogen bonds; the carbonyl oxygens and the nearest-neighbor alpha-hydrogens also took more favorable relative positions.     

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.     

Design of peptides with branched beta-carbon dehydro-residues: syntheses, crystal structures and molecular conformations of two peptides, (I) N-Carbobenzoxy-DeltaVal-Ala-Leu-OCH3 and (II) N-Carbobenzoxy-DeltaIle-Ala-Leu-OCH3.

Highly specific structures can be designed by inserting dehydro-residues into peptide sequences. The conformational preferences of branched beta-carbon residues are known to be different from other residues. As an implication it was expected that the branched beta-carbon dehydro-residues would also induce different conformations when substituted in peptides. So far, the design of peptides with branched beta-carbon dehydro-residues at (i + 1) position has not been reported. It may be recalled that the nonbranched beta-carbon residues induced beta-turn II conformation when placed at (i + 2) position while branched beta-carbon residues induced beta-turn III conformation. However, the conformation of a peptide with a nonbranched beta-carbon residue when placed at (i + 1) position was not found to be unique as it depended on the stereochemical nature of its neighbouring residues. Therefore, in order to induce predictably unique structures with dehydro-residues at (i + 1) position, we have introduced branched beta-carbon dehydro-residues instead of nonbranched beta-carbon residues and synthesized two peptides: (I) N-Carbobenzoxy-DeltaVal-Ala-Leu-OCH3 and (II) N-Carbobenzoxy-DeltaIle-Ala-Leu-OCH3 with DeltaVal and DeltaIle, respectively. The crystal structures of peptides (I) and (II) have been determined and refined to R-factors of 0.065 and 0.063, respectively. The structures of both peptides were essentially similar. Both peptides adopted type II beta-turn conformations with torsion angles; (I): phi1 = -38.7 (4) degrees, psi1 = 126.0 (3) degrees; phi2 = 91.6 (3) degrees, psi2 = -9.5 (4) degrees and (II): phi1 = -37.0 (6) degrees, psi1 = 123.6 (4) degrees, phi2 = 93.4 (4), psi2 = -11.0(4) degrees respectively. Both peptide structures were stabilized by intramolecular 4-->1 hydrogen bonds. The molecular packing in both crystal structures were stabilized in each by two identical hydrogen bonds N1...O1' (-x, y + 1/2, -z) and N2...O2' (-x + 1, y + 1/2, -z) and van der Waals interactions.     

Conformation and hydrogen bonding of N-formylpeptides: crystal and molecular structure of N-formyl-L-alanyl-L-aspartic acid.

Crystals of N-formyl-L-alanyl-L-aspartic acid (C8H11N2O6) grown from aqueous methanol solution are orthorhombic, space group, P2(1)2(1)2(1) with cell parameters at 294K of a = 13.619(2), b = 8.567(2), c = 9.583(3)A, V = 1118.1A3, M.W. = 232.2, Z = 4, Dm = 1.38 g/cm3 and Dx = 1.378 g/cm3. The crystal structure was solved by the application of direct methods and refined to an R value of 0.075 for 1244 reflections with I greater than or equal to 3 sigma collected on a CAD-4 diffractometer. The structure contains two short intermolecular hydrogen bonds: (i) between the C-terminal carboxyl OH and the N-acyl oxygen (2.624(3)A), a characteristic feature found in many N-acyl peptides and (ii) between the aspartic carboxyl OH. and the peptide oxygen OP1 (2.623(3)A). The peptide is nonplanar (omega = 165.5(6) degrees). The molecule takes up a folded conformation in contrast to N-formyl peptides which form extended beta-sheets; the values of phi 1, psi 1, phi 2, psi 2(1), and psi 2(2) are, respectively -65.7(6), 152.0(5), -107.2(5), 30.9(5), and -150.3(6). The aspartic acid side chain conformation is g- with chi 1 = 73.1(5). The formyl group, as expected, is transplanar [OF-CF-N1-CA1 = -4.0(8) degrees]. The presence of the short O-H ... O hydrogen bond emerges as a structural feature common to this peptide and several other N-formyl peptides. There are no C-H ... O hydrogen bonds in this structure.     

Entrapping unusual folding characteristics of the beta-Ala residues in a model peptide: Boc-beta-Ala-Aib-beta-Ala-NHCH3.

Crystal structure analysis of a model peptide: Boc-beta-Ala-Aib-beta-Ala-NHCH3 (beta-Ala: 3-amino propionic acid; Aib: alpha-aminoisobutyric acid) revealed distinct conformational preferences for folded [phi approximately 136 degrees, mu approximately -62 degrees, psi approximately 100 degrees] and semifolded [phi approximately 83 degrees, mu approximately -177 degrees, psi approximately -117 degrees] structures of the N-and C-terminus beta-Ala residues, respectively. The overall folded conformation is stabilized by unusual Ni...H-Ni+1 and nonconventional C-H...O intramolecular hydrogen bonding interactions.     

Crystal structure and conformation of a highly constrained linear tetrapeptide Boc-Leu-dehydro Phe-Ala-Leu-OCH3.

The conformation of a tetrapeptide containing a dehydro amino acid, delta ZPhe, in its sequence has been determined in the crystalline state using X-ray crystallographic techniques. The tetrapeptide, Boc-Leu-delta ZPhe-Ala-Leu-OCH3, crystallizes in the orthorhombic space group P2(1)2(1)2(1) with four molecules in a unit cell of dimensions a = 11.655(1) A, b = 15.698(6) A and c = 18.651(3) A V = 3414.9 A and Dcalc = 1.12 g/cm-3. The asymmetric unit contains one tetrapeptide molecule, C30H46N4O7, a total of 41 nonhydrogen atoms. The structure was determined using the direct methods program SHELXS86 and refined to an R-factor of 0.049 for 3347 reflections (I3.0(I). The linear tetrapeptide in the crystal exhibits a double bend of the Type III-I, with Leu1 (phi = -54.1 degrees, psi = -34.5 degrees) and delta ZPhe2 (phi = -59.9 degrees, psi = -17.1 degrees) as the corner residues of Type III turn and delta ZPhe2 (phi = -59.9 degrees, psi = -17.1 degrees) and Ala3 (phi = -80.4 degrees, psi = 0.5 degrees) residues occupying the corners of Type I turn, with delta ZPhe as the common residue in the double bend. The turn structures are further stabilized by two intramolecular 4----1 type hydrogen bonds.     

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.     

Conformation and hydrogen bonding of N-formylmethionyl peptides. Parallel beta-sheet in the crystal structure of N-formyl-L-methionyl-L-valine

Crystals of N-formyl-L-methionyl-L-valine (C11H20N2O)4S, M.W. = 276.3) are orthorhombic, space group )2(1)2(1)2(1) with cell constants at 294K of a = 4.851 (1), b = 14.925 (1), c = 19.745 (3) A, V = 1429.8 (1) A3, Z = 4 and observed (Dm) and calculated (Dx) of 1.49 and 1.488 g x cm-3, respectively. The crystal structure was solved using automatic diffractometer data (1260 reflections larger than or equal to 3 sigma) and refined to a final R-value of 0.035. This structure contains a short (2.626 (3) A) intermolecular hydrogen bond between the carboxyl OH and the N-acyl oxygen, a feature common to most N-acylamino acids and N-acylpeptides. The peptide is nearly planar (omega = 174.6 (5)); the values of psi 1, phi 2, psi 1T and psi 2T are, respectively, 131.8 (4) degrees, -139.9 (5) degrees, -39.3 (4) degrees and 142.1 (4) degrees. The methionine side chain is not zig-zag transplanar; the side chain torsion angles are: chi 1(1) = -60.0 (4) degrees, chi 2(1) = 176.0 (4) degrees and chi 3(1) = 71.8 (4) degrees. The two C gamma's for valine have psi 1-values of -64.4 (5) degrees and 173.7 (5) degrees. The formation of the parallel rather than antiparallel beta-sheet structure, the participation of the N-formyl group in the parallel beta-sheet and the use of C-H ... O hydrogen bonds to stabilize the beta-sheet are novel features found in this structure.     

Design of peptides with alpha,beta-dehydro-residues: synthesis, and crystal and molecular structure of a 3(10)-helical tetrapeptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3.

The peptide Boc-L-Val-deltaPhe-deltaPhe-L-Ile-OCH3 was synthesized using the azlactone method in the solution phase, and its crystal and molecular structures were determined by X-ray diffraction. Single crystals were grown by slow evaporation from solution in methanol at 25 degrees C. The crystals belong to an orthorhombic space group P2(1)2(1)2(1) with a = 12.882(7) A, b = 15.430(5) A, c = 18.330(5) A and Z = 4. The structure was determined by direct methods and refined by a least-squares procedure to an R-value of 0.073. The peptide adopts a right-handed 3(10)-helical conformation with backbone torsion angles: phi1 = 56.0(6)degrees, psi1 = -38.0(6)degrees, phi2 = -53.8(6)degrees, psi2 = 23.6(6)degrees, phi3 = -82.9(6)degrees, psi3 = -10.6(7)degrees, phi4 = 124.9(5)degrees. All the peptide bonds are trans. The conformation is stabilized by intramolecular 4-->1 hydrogen bonds involving Boc carbonyl oxygen and NH of deltaPhe3 and CO of Val1 and NH of Ile4. It is noteworthy that the two other chemically very similar peptides: Boc-Val-deltaPhe-deltaPhe-Ala-OCH3 (i) and Boc-Val-deltaPhe-deltaPhe-Val-OCH3 (ii) with differences only at the fourth position have been found to adopt folded conformations with two overlapping beta-turns of types II and III', respectively, whereas the present peptide adopts two overlapping beta-turns of type III. Thus the introduction of Ile at fourth position in a sequence Val-deltaPhe-deltaPhe-X results in the formation of a 3(10)-helix. The crystal structure is stabilized by intermolecular hydrogen bonds involving NH of Val1 and carbonyl oxygen of a symmetry related (-x, y - 1/2, 1/2 + z) deltaPhe2 and NH of deltaPhe2 with carbonyl oxygen of a symmetry related (x, y1/2, 1/2 + z) Ile4. This gives rise to long columns of helical molecules linked head to tail running along [010] direction.     

Molecular orbital studies on nucleoside analogs. II. Conformation of 6-azapyrimidine nucleosides.

PCILO (Perturbative Configuration Interaction using Localised Orbitals) computations have been carried out for three 6-azapyrimidine nucleosides, 6-azauridine, 6-azacytidine and 6-azathymidine, for both C(2')-endo and C(3')-endo pucker of the sugar ring. The results indicate a syn (chiCN=180 degrees) conformation followed by chiCN=90 degrees and gg conformation for C(3')-endo 6-aza analogs as compareed to the anti (chiCN=0 degrees) and gg conformation preferred by the corresponding pyrimidine nucleosides. For C(2')-endo sugar geometry, 6-azauridine and 6-azacytidine prefer, respectively, chiCN=0 degrees (anti) and phi C(4')-C(5')=60 degrees C (gg) and chiCN-240 degrees (syn) and phi C(4')-C(5')=120 degrees. The corresponding nucleosides, uridine and cytidine, show a preference for syn (chiCN=240 degrees) and gg and anti(chiCN=0 degrees) and gg , respectively. The X-ray crystallographic conformations of 6-azauridine and 6-azacytidine have been attributed to intermolecular hydrogen bonding and crystal packing forces. The results of PMR, CD and ORD studies on 6-azauridine and 6-azacytidine in aqueous solutions are in agreement with the PCILO predictions.     

Linkage and pyranosyl ring twisting in cyclodextrins

Acylated beta-cyclodextrins (beta-CDs) were studied to gain perspective on maltose octapropanoate, the crystal structure of which was reported in the preceding paper in this issue. Acylated beta-CDs are distorted so we looked at other CDs and gained increased understanding of distortion in CDs and possibly, shapes in starch. Classic CDs have six to eight glucose residues in a doughnut shape that is stabilized by a ring of inter-residue O3,,,O2' hydrogen bonds. On a phi,psi energy map for a maltose analog that does not form hydrogen bonds, classic CD linkages have higher energies than structures that are stabilized by the exo-anomeric effect. In distorted beta-CDs, which lack hydrogen bonding, some linkages attain low-energies from the exo-anomeric effect and acyl stacking. Those linkages result in left-handed helical geometry so other linkages are forced by the CD macrocycle to have counter-balancing right-handed character. Permethylated gamma-CDs have two 'flipping' linkages as do some larger native CDs. Flipping linkages allow two left-handed segments to join into a macrocycle, thus avoiding the higher-energy, right-handed forms. Some glucose rings in derivatized beta-CDs have substantial positive twists of the pseudo torsion angle O1-C1...C4-O4, adding right-handed character to balance the left-handed linkages. In substituted gamma-CD, all residues have negative twists, giving extra left-handed character to the short, pseudo-helical segments. In non-macrocyclic molecules the twists ranged from -14 degrees to +2 degrees , averaging -6.1 degrees. In these beta- and gamma-CDs, the twists ranged from -22 degrees to +16 degrees for (4)C(1) rings, and the (O)S(2) ring in acetylated beta-CD has a twist of +34 degrees . Glucose residues in other CDs were less twisted.     

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

The peptide N-Ac-dehydro-Phe-L-Val-OH (C16H20N2O4) was synthesized by the usual workup procedure. The peptide crystallizes from its solution in acetonitrile at 4 degrees in hexagonal space group P6(5) with a = b = 11.874(2)A, c = 21.856(9) A, V = 2668(1) A3, Z = 6, dm = 1.151(3) g cm-3, dc = 1.136(4) g cm-3, CuK alpha = 1.5418 A, mu = 0.641 mm-1, F(000) = 972, T = 293 K. The structure was solved by direct methods and refined by least-squares procedure to an R value of 0.074 for 1922 observed reflections. In the dehydro-residue, the C1 alpha-C1 beta distance is 1.35(1) A while the bond angle C1 alpha-C1 beta-C1 gamma is 131.2(9) degrees. The backbone torsion angles are: omega 0 = 172(1) degrees, phi 1 = -60(2) degrees, psi 1 = -31(2) degrees, omega 1 = -179(1) degrees, phi 2 = 59(2) degrees. These values suggest that the peptide tends to adopt an alternating right-handed and left-handed helical conformation. The side chain torsion angles are: chi 1(1) = -6(2) degrees, chi 1(2.1) = -1(2) degrees, chi 1(2.2) = -178(2) degrees, chi 2(1.1) = 63(2) degrees and chi 2(1.2) = -173(1) degrees. These values show that the side chain of dehydro-Phe is planar whereas the valyl side chain adopts a sterically most preferred conformation. The molecules, linked by intermolecular hydrogen bonds and van der Waals forces, are arranged in helices along the c-axis. The helices are held side-by-side by van der Waals contacts.     

Crystal and molecular structure of methyl 4-O-methyl-beta-D-glucopyranosyl-(1-->4)-beta-D-glucopyranoside

The cellulose model compound methyl 4-O-methyl-beta-D-glucopyranosyl-(1-->4)-beta-D-glucopyranoside (6) was synthesised in high overall yield from methyl beta-D-cellobioside. The compound was crystallised from methanol to give colourless prisms, and the crystal structure was determined. The monoclinic space group is P2(1) with Z=2 and unit cell parameters a=6.6060 (13), b=14.074 (3), c=9.3180 (19) A, beta=108.95(3) degrees. The structure was solved by direct methods and refined to R=0.0286 for 2528 reflections. Both glucopyranoses occur in the 4C(1) chair conformation with endocyclic bond angles in the range of standard values. The relative orientation of both units described by the interglycosidic torsional angles [phi (O-5' [bond] C-1' [bond] O-4 [bond] C-4) -89.1 degrees, Phi (C-1' [bond] O-4 [bond] C-4 [bond] C-5) -152.0 degrees] is responsible for the very flat shape of the molecule and is similar to those found in other cellodextrins. Different rotamers at the exocyclic hydroxymethyl group for both units are present. The hydroxymethyl group of the terminal glucose moiety displays a gauche-trans orientation, whereas the side chain of the reducing unit occurs in a gauche-gauche conformation. The solid state (13)C NMR spectrum of compound 6 exhibits all 14 carbon resonances. By using different cross polarisation times, the resonances of the two methyl groups and C-6 carbons can easily be distinguished. Distinct differences of the C-1 and C-4 chemical shifts in the solid and liquid states are found.     

Role of a two-residue spacer in an alpha,beta-Didehydrophenylalanine containing hexapeptide: crystal and solution structure of Boc-val-deltaPhe-Leu-Ala-deltaPhe-Ala-OMe.

The peptide Boc-Val1-deltaPhe2-Leu3-Ala4-deltaPhe5-Ala6-OMe has been examined for the structural consequence of placing a two-residue segment between the deltaPhe residues. The peptide is stabilized by four consecutive beta-turns. The overall conformation of the molecule is a right-handed 3(10)-helix, with average (phi, psi) values (-67.7 degrees, -22.7 degrees), unwound at the C-terminus. The 1H NMR results also suggest that the peptide maintains its 3(10)-helical structure in solution as observed in the crystal state. The crystal structure is stabilized through head-to-tail hydrogen bonds and a repertoire of aromatic interactions laterally directed between adjacent helices, which are antiparallel to each other. The aromatic ring of deltaPhe5 forms the hub of multicentred interactions, namely as a donor in aromatic C-H...pi and aromatic C-H...O=C interactions and as an acceptor in a CH3...pi interaction. The present structure uniquely illustrates the unusual capability of a deltaPhe ring to host such concerted interactions and suggests its exploitation in introducing long-range interactions in the folding of supersecondary structures.     

The crystal structure of lithium L-ascorbate dihydrate.

The crystal structure of lithium L-ascorbate dihydrate is triclinic, Pl; with a = 5.964(9), b = 5.299(9), c = 7.760(15) A; alpha = 100.82(9), beta = 109.78(9), gamma = 92.02(9) degrees. The plant fragment of the ascorbate anion is a part of the five-membered ring [C-1,C-2,C-3(O-3),C-4], and O-4 deviates by 0.053(2) A from this plane. Deprotonated O-3 is an acceptor of three hydrogen bonds, but does not interact with Li+. The coordination number of the Li+ is 5 and it is bonded to two water molecules and three hydroxyl oxygen atoms of two ascorbate anions: O-2 and the gauche O-5, 6 of the side chain.     

Octa-O-propanoyl-beta-maltose: crystal structure, acyl stacking, related structures, and conformational analysis

The crystal structure of beta-maltose octapropanoate (1) was solved to improve understanding of di-, oligo-, and polysaccharide conformations. The O6 and O6' atoms are in gg and gt orientations, respectively. Extrapolation of the coordinates of the non-reducing residue and observed linkage bond and torsion angles of 1 [Formula: see text] yields a left-handed helix similar to amylose triacetate I. The phi and psi values of 1 are also similar to those of other crystalline, acylated maltose compounds as well as some hydroxyl-bearing molecules. Acylated maltose moieties are often stabilized by stacking of the carbonyl groups and alpha-carbons on O3 and O2' as well as by the exo-anomeric effect. The conformation of 1 is within the 1-kcal/mol contour on a hybrid energy map built with a dielectric constant of 7.5, but corresponds to higher energies on maps made with lower dielectric constants. In one region of phi,psi space, both hydroxyl-bearing and derivatized maltose moieties are found but no inter-residue, intramolecular hydrogen-bonding occurs. In another region, only hydroxyl-bearing molecules crystallize and O2'...O3 hydrogen bonds are always found. In agreement with the energy surfaces, amylose helices extrapolated from available linkage geometries were almost all left-handed.     

X-ray structure determination and modeling of the cyclic tetrasaccharide cyclo

The cyclic tetrasaccharide cyclo-[-->6)-alpha-D-Glcp-(1-->3)-alpha-D-Glcp-(1-->6)-alpha-D-Glcp-(1-->3)-alpha-D-Glcp-(1-->] is the major compound obtained by the action of endo-alternases on the alternan polysaccharide. Crystals of this cyclo-tetra-glucose belong to the orthorhombic space group P2(1)2(1)2(1) with a = 7.620(5), b = 12.450(5) and c = 34.800(5) A. The asymmetric unit contains one tetrasaccharide together with five water molecules. The tetrasaccharide adopts a plate-like overall shape with a very shallow depression on one side. The shape is not fully symmetrical and this is clearly apparent on comparing the (phi, psi) torsion angles of the two alpha-(1-->6) linkages. There is almost 10 degrees differences in phi and more than 20 degrees differences in psi. The hydrogen bond network is asymmetric, with a single intramolecular hydrogen bond: O-2 of glucose ring 1 being the donor to O-2 of glucose ring 3. These two hydroxyl groups are located below the ring and their orientation, dictated by this hydrogen bond, makes the floor of the plate. Among the five water molecules, one located above the center of the plate occupies perfectly the shallow depression in the plate shape formed by the tetrasaccharide. Molecular dynamics simulation of the tetrasaccharide in explicit water allows rationalization of the discrepancies observed between the X-ray structures and data obtained previously by NMR.