Conformational studies on the selectin and natural killer cell receptor ligands sulfo- and sialyl-lacto-N-fucopentaoses (SuLNFPII and SLNFPII) using NMR spectroscopy and molecular dynamics simulations. Comparisons with the nonacidic parent molecule LNFPII

This investigation is focused on the conformational behavior of the blood group Lewisa (Le(a)-active pentasaccharide lacto-N-fucopentaose II (LNFPII) and its sulfated and sialylated analogs, SuLNFPII and SLNFPII. The latter two are more potent oligosaccharide ligands for the animal lectins, E- and L-selectin, and the natural killer cell receptor, NKR-P1, than are the shorter chain analogs based on the trisaccharide Le(a) domain. We report here that the three oligosaccharides based on the fucopentasaccharide have very similar average solution conformations as determined from NMR spectroscopical parameters, in particular 13C chemical shift differences. From restrained simulated annealing and restrained molecular dynamics (MD) simulations performed in order to determine the most probable conformational distributions around the glycosidic linkages we derive models for these oligosaccharides that are in good agreement with experimental parameters, such as rotating-frame Overhauser effects (ROE's) and long-range 1H,13C coupling constants across the glycosidic linkages. In these model structures the Le(a) domain at the non-reducing end of the longer chain oligosaccharides approximates the same rigid structure as in the shorter analogs. The Gal beta 1-4Glc linkage at the reducing end is also rather rigid, showing only little more flexibility than the Le(a) domain. However, the NeuAc alpha 2-3Gal linkage in SLNFPII, and the GlcNAc beta 1-3Gal linkage in all three oligosaccharides are flexible, in each case fluctuating mainly between two minimum energy structures: (phi = -81 degrees, psi = 8 degrees) and (phi = -160 degrees, psi = -20 degrees) for the NeuAc alpha 2-3Gal linkage, as reported previously for the isomeric sequence 3'-sialyl Le(x), and (phi = -25 degrees, psi = -26 degrees) and (phi = 20 degrees, psi = 24 degrees) for the GlcNAc beta 1-3Gal linkage. The flexibility of the latter linkage may allow the lactosyl domain at the reducing end to fit with little strain into extended carbohydrate binding sites on the recognition proteins, and, for the purposes of drug designs, it will be important to establish which conformational distribution is assumed for the GlcNAc beta 1-3Gal linkage in these longer chain oligosaccharides in the bound state.     

The aqueous solution structure of a lipoteichoic acid from Streptococcus pneumoniae strain R6 containing 2,4-diamino-2,4,6-trideoxy-galactose: evidence for conformational mobility of the galactopyranose ring

The 2D-NOESY spectra for the per-N-acetylated and the native lipoteichoic acid (LTA) oligomer from Streptococcus pneumoniae strain R6 clearly indicate a difference in conformation of the 2,4,6-trideoxy-galactopyranose ring. Whereas the 2,4-N-acetylated Gal24N adopts the usual 4C1 chair conformation, the native 2-N-acetyl-4-amino Gal24N exhibits conformational mobility with comparable populations in the 4C1 chair and 5S1 skew conformations, as determined using MD simulation for the partial trisaccharide Me-beta-D-Glc6P-(1-->3)-alpha-D-Gal24N-[6-PC]-(1-->4)-alpha- D-galNAc and from the intra-ring NOE effects. 31P-NMR spectra point to a strong electrostatic or hydrogen-bonding interaction between the free 4-NH2 group on the Gal24N and the negatively charged diester phosphate group between adjacent pentasaccharide repeating-units [Ribitol-(5-->6)-beta-D-Glc6P]. Molecular modelling and MD simulation experiments confirmed that such an interaction was feasible with the Gal24N galactopyranose ring in the inverted B1.4 or skew 5S1 conformation.     

Prediction of conformational states of amino acids using a Ramachandran plot

(phi, psi) data from crystal structures of 221 proteins having high resolution and sequence similarity cut-off at the 25% level were analysed by dividing the Ramachandran plot in three regions representing three conformational states: (i) conformational state 1: conformations in the (phi, psi) range from (-140 degrees, -100 degrees) to (0 degrees, 0 degrees); (ii) conformational state 2: conformations with (phi, psi) from (-180 degrees, 80 degrees) to (0 degrees, 180 degrees); and (iii) conformational state 3: all the remaining conformations in the (phi, psi) plane which are not included in the above two conformational states. Normalized probability values of the occurrence of single amino acid residues in conformational regions 1-3 and similar values for dipeptides were calculated. Comparisons of single residue and dipeptide normalized probability values have shown that short-range interactions, although strong, destabilize conformational states of only 44 dipeptides out of the 400 x 9 possible states. However, dipeptide frequency values provide better resolving power than single-residue potentials when used to predict conformational states of residues in a protein from its primary structure. The simple approach used in the present study to predict conformational states yields an accuracy of > 70% for 14 proteins and an accuracy in the range of 50-70% for 247 proteins. Thus these studies point out yet another use of the Ramachandran plot and the role of tertiary interactions in protein folding.     

Chain conformational analysis of beijeran by n-h map calculations

Possible regular helix models of beijeran, a new acidic heteropolysaccharide consisting of a trisaccharide as a repeating unit, were investigated. Conformational analyses of the three component disaccharides were first carried out by calculating their relaxed-residue energy maps with respect to the glycosidic bond rotations, phi and psi. A search for possible beijeran chain conformations was carried out by calculating the two-dimensional map of the helix parameters; n (the number of asymmetric units per a fiber repeat) and h (the axial rise per the unit), on the basis of the phi-psi conformations taken from the low energy regions of each of the three energy maps. The n-h values of the helix models with low steric energies were mostly found to be around the experimental values (n = 2 and h = 1.20-1.25 nm), which may support the present methodology. It was also suggested that the internal flexibility of beijeran chain allowed it to conform in diverse helical structures, each of which were reasonably in accord with the observed n-h values. The three representative helix models were finally proposed for the beijeran chain conformation in the crystal structure.     

Differential deuterium isotope shifts and one-bond 1H-13C scalar couplings in the conformational analysis of protein glycine residues

The one-bond deuterium isotope shift effect for glycine C alpha resonances exhibits a conformational dependence comparable to that of the corresponding 1JHC scalar coupling in both magnitude (approximately 11 Hz at 14.1 T) and dihedral angle dependence. The similarity in the conformational dependence of the 1JHC and deuterium isotope shift values suggests a common physical basis. Given the known distribution of (phi, psi) main-chain dihedral angles for glycine residues, the deuterium isotope shifts and the 1JHC scalar couplings can determine conformations in the left- and right-handed helical-to-bridge regions of the (phi, psi) plane to an accuracy of approximately 13 degrees. In the absence of stereochemical assignments, the differential deuterium isotope shifts and the 1JHC scalar couplings can be combined with limited independent structural information (e.g., the sign of phi) to determine the chirality of the deuterium substitution.     

Orientation of the saccharide chains of glycolipids at the membrane surface: conformational analysis of the glucose-ceramide and the glucose-glyceride linkages using molecular mechanics (MM3)

Preferred conformations of the saccharide-ceramide linkage of glucosylceramides with different ceramide structures (normal and hydroxy fatty acids) were investigated by molecular mechanics (MM3) calculations and compared with conformational features obtained for glucosylglycerolipids (diacyl and dialkyl analogues). Relaxed energy map calculations with MM3 were performed for the three bonds (C1'-O1-C1-C2, torsion angles phi, psi, and theta 1) of the glucose-ceramide/diglyceride linkage at different values of the dielectric constant. For the phi torsion of the glycosidic C1'-O1 bond the calculations show a strict preference for the +sc range whereas the psi/theta 1 energy surface is dependent on the structure of the lipid moiety as well as on the dielectric constant (epsilon). Calculations performed on glucosylceramide with normal and hydroxy fatty acids at epsilon = 4 (bilayer subsurface conditions) show three dominating conformers (psi/theta 1 = ap/-sc, -sc/ap, and ap/ap). The ap/-sc conformer, which represents the global energy minimum, is stabilized by polar interactions involving the amide group. The +sc rotamer of theta 1 is unfavored in sphingolipids due to a Hassel-Ottar effect involving the sphingosine O3 and O1 oxygen atoms. Comparative calculations on glycosylglycerolipid analogues (ester and ether derivatives) show a distinct preference for the ap rotamer of theta 1. An evaluation of the steric hindrance imposed by the surrounding membrane surface shows that in a bilayer arrangement the range of possible conformations for the saccharide-lipid linkage is considerably reduced. The significance of preferred conformations of the saccharide-ceramide linkage for the presentation and recognition of the saccharide chains of glycosphingolipids at the membrane surface is discussed.     

Coexistence of folded and extended conformations of a tripeptide containing alpha, alpha -di-n-propylglycine in crystals

The crystal structure of the tripeptide Boc-Leu-Dpg-Val-OMe (Dpg, alpha, alpha -di-n-propylglycine) reveals the coexistence of two distinct backbone conformations. In molecule A the Dpg residue adopts a fully extended conformation (phi = 76.0 degrees, psi = 180.0 degrees) while in molecule B a left handed helical conformation (phi = 62.8 degrees, psi = 39.6 degrees) is observed. Molecule B adopts a folded structure corresponding to a highly distorted Type II beta-turn conformation, which lacks an intramolecular 4 -> 1 hydrogen bond. In contrast, molecule A has an open, extended conformation. The results demonstrate that both fully extended and helical conformations are energetically accessible to the Dpg residue.     

Design of peptides using alpha,beta-dehydro-residues: synthesis, crystal structure and molecular conformation of Boc-L-Val-delta Phe-delta Phe-L-Val-OCH3

The peptide Boc-L-Val-delta Phe-delta Phe-L-Val-OCH3 was synthesized by the azlactone method in solution phase, and its crystal and molecular structures were determined by x-ray diffraction method. Single crystals were grown by slow evaporation from a methanol/water solution at 6 degrees C. The crystals belong to an orthorhombic space group P212121 with a = 10.478 (6) A, b = 13.953 (I), c = 24.347 (2) and Z = 4. The structure was determined by direct methods and refined by least squares procedure to an R value of 0.052. The structure consists of a peptide and a water molecule. The peptide adopts two overlapping beta-turn conformations of Types II and I' with torsion angles: phi 1 = -54.8 (6) psi 1 = 130.5 (4), phi 2 = 65.8 (5), psi 2 = 12.8 (6), phi 3 = 79.4 (5), psi 3 = 3.9 (7) degrees. The conformation is stabilized by intramolecular hydrogen bonds involving Boc CO and NH of delta Phe3 and CO of Val1 and NH of Val4. The molecules are tightly packed in the unit cell. The crystal structure is stabilized by hydrogen bonds involving NH of delta Phe2 and CO of a symmetry related (x-1/2, 1/2-y, -z) delta Phe2. The solvent-water molecule forms two hydrogen bonds with peptide molecule involving NH of Val1 as an acceptor and another with CO of a symmetry related (1-x, y-1/2, 1/2 -z) delta Phe3 as a donor. These studies indicate that a tetrapeptide with two consecutive delta Phe residues sequenced with valines on both ends adopts two overlapping beta-turns of Types II and I'.     

Management of chronic myeloid leukaemia

A tetrasaccharide related to the blood group oligosaccharides, known as sialyl LewisX, has been proposed as the receptor for the lectin responsible for leukocyte adhesion named alternatively as E-selectin or ELAM-1. The 13C- and 1H-nmr spectra have been completely assigned for a tetrasaccharide model of this receptor, Neu5Ac alpha-(2-->3)-Gal beta-(1-->4)-[Fuc alpha-(1-->3)-]GlcNAc beta-NHAc. Quantitative nuclear Overhauser data (NOESY) have been recorded and analyzed by a complete spin matrix simulation method. Conformational space was exhaustively searched and all conformational models whose simulated NOESY spectra matched the experiment were found. Molecular mechanics and molecular dynamics calculations were carried out to test whether the experimental conformations are low energy and thus likely to represent true single conformations for the tetrasaccharide. It was concluded that while the LewisX trisaccharide portion of the compound adopts a single conformation, there is likely to be some flexibility about the Neu5Ac alpha-(2-->3)-linkage. A model featuring fast exchange between two different conformations of this linkage is found to be consistent with both the nmr experiments and the molecular dynamics simulations.     

(13C)-substituted sucrose: 13C-1H and 13C-13C spin coupling constants to assess furanose ring and glycosidic bond conformations in aqueous solution

Sucrose (beta-D-fructofuranosyl alpha-D-glucopyranoside, 1), methyl alpha-D-fructofuranoside (2), and methyl beta-D-fructofuranoside (3) have been prepared by chemical and/or enzymic methods with single sites of 13C-substitution at C-1, C-2, C-3, and C-6 of the fructofuranosyl ring. 1H (500 MHz) and 13C (75 and 125 MHz) NMR spectra of 1-3 have been obtained, yielding 1H-1H, 13C-1H, and 13C-13C spin coupling constants that were used to assess furanose ring and glycoside bond conformations in aqueous (2H2O) solution. Results show that the conformational mobility of the furanosyl ring in 3 is altered when incorporated into 1. Furthermore, 13C-13C and 13C-1H spin couplings across the glycosidic linkage suggest a psi torsion angle different from that observed in the crystal (phi appears similar). Interplay between the strength of the exoanomeric effect and hydrogen bonding in solution may be responsible, in part, for the apparent conformational flexibility of 1. In addition, spin couplings in 2 and 3 have been compared to those measured previously in alpha-D-threo-pentulofuranose (4) and beta-D-threo-pentulofuranose (5), respectively, as a means to study the effect of glycosidation and hydroxymethyl substitution on the solution conformation of the 2-ketofuranose ring. The conversion of 4 to 2 is accompanied by minimal conformational change, whereas a significant change accompanies the conversion of 5 to 3, showing that the effect of substitution on ring conformation depends highly on ring configuration before and after substitution.     

Solution studies of isepamicin and conformational comparisons between isepamicin and butirosin A when bound to an aminoglycoside 6'-N-acetyltransferase determined by NMR spectroscopy

NMR spectroscopy, combined with molecular modeling, was used to determine the conformations of isepamicin and butirosin A in the active site of aminoglycoside 6'-N-acetyltransferase-Ii [AAC-(6')-Ii]. The results suggest two enzyme-bound conformers for isepamicin and one for butirosin A. The dihedral angles that describe the glycosidic linkage between the A and B rings for the two conformers of AAC(6')-Ii-bound isepamicin were phi AB = -7.9 +/- 2.0 degrees and psi AB = -46.2 +/- 0.6 degrees for conformer 1 and phi AB = -69.4 +/- 2.0 degrees and psi AB = -57.7 +/- 0.5 degrees for conformer 2. Unrestrained molecular dynamics calculations showed that these distinct conformers are capable of interconversion at 300 K. When superimposed at the 2-deoxystreptamine ring, one enzyme-bound conformer of isepamicin (conformer 1) places the reactive 6' nitrogen in a similar position as that of butirosin A. Conformer 2 of AAC(6')-Ii-bound isepamicin may represent an unproductive binding mode. Unproductive binding modes (to aminoglycoside modifying enzymes) could provide one reason isepamicin remains one of the more effective aminoglycoside antibiotics. The enzyme-bound conformation of butirosin A yielded an orthogonal arrangement of the 2,6-diamino-2,6-dideoxy-D-glucose and D-xylose rings, as opposed to the parallel arrangement which was observed for this aminoglycoside in the active site of an aminoglycoside 3'-O-phosphotransferase [Cox, J. R., and Serpersu, E. H. (1997) Biochemistry 36, 2353-2359]. The complete proton and carbon NMR assignments of the aminoglycoside antibiotic isepamicin at pH 6.8 as well as the pKa values for it's amino groups are also reported.     

The pseudo-beta I-turn. A new structural motif with a cis peptide bond in cyclic hexapeptides

Synthesis and conformational analysis of three cyclic hexapeptides cyclo(-Gly1-Pro2-Phe3-Val4-Xaa5-Phe6), Xaa = Phe (I), D-Phe (II) and D-Pro (III), were carried out to examine the influence of proline on the formation of reverse turns and the dynamics of hydrophobic peptide regions. Assignment of all 1H and 13C resonances was achieved by homo- and heteronuclear 2D-NMR techniques (TOCSY, ROESY, HMQC, HMQC-TOCSY and HMBCS-270). The conformational analysis is based on interproton distances derived from ROESY spectra and homo- and heteronuclear coupling constants (E.COSY, HETLOC and HMBCS-270). For structural refinements restrained molecular dynamics (MD) simulations in vacuo and in DMSO were performed. Each peptide exhibits two conformations in DMSO solution due to cis-trans isomerism about the Gly-Pro peptide bond. Surprisingly the cis-Gly-Pro segment in the minor isomers is not involved in a beta VI-turn, but forms a turn structure with cis-Gly-Pro in the i and i + 1 positions. Although no stabilizing hydrogen bond is found in this turn, the phi- and psi-angles closely correspond to a beta I-turn [Pro2: phi(i + 1) -60 degrees, psi(i + 1) -30 degrees; Phe3: phi(i + 2) -100 degrees, psi(i + 2) -50 degrees]. Hence we call this structural element a pseudo-beta I-turn. As expected, in the dominating all-trans isomers proline occupies the i + 1 position of a standard beta I-turn. Therefore, cis-trans isomerization of the Gly1-Pro2 amide bond only induces a local conformational rearrangement, with minor structural changes in other parts of the molecule. However, the geometry of the other regions is affected by the chirality of the i + 1 amino acid for both isomers (beta I for Phe5, beta II' for D-Phe5 or D-Pro5).     

Conformational analysis of methyl 6-O-[(R)- and (S)-1-carboxyethyl]-alpha-D-galactopyranoside by MM and Langevin dynamics simulations

The conformational space of methyl 6-O-[(R)- and (S)-1-carboxyethyl]-alpha-D-galactopyranoside has been investigated. A grid search employing energy minimization at each grid point over the three major degrees of freedom, namely phi, psi and omega, identified low energy regions. The R-isomer shows five low energy conformers within ca. 1 kcal mol(-1) of the global energy minimum. The S-isomer has two conformers within a few tenths of a kcal mol(-1) of the global energy minimum. Langevin dynamics simulations have been have been performed at 300 K for 30 ns of each isomer. The phi dihedral angle has as its major conformer (g-) for the R-isomer whereas it is the (g+) conformer for the S-isomer. For the psi dihedral angle the (t) conformer has the highest population for both isomers. The dihedral angle omega has the (g+) conformer most highly populated, both for the R- and S-isomer. The above five and two conformational states for the R- and S-isomers, respectively, make up 90% in each case of the populated states during the Langevin dynamics (LD) simulations. Rate constants for the omega dihedral angle have been calculated based on a number correlation function. Three bond homo- and heteronuclear, i.e. proton and carbon-13, coupling constants have been calculated from the dynamics trajectories for comparison to experimental values. The heteronuclear coupling constant H2',C6 has been measured for the S-isomer and found to be 3.3 Hz. The J value calculated from the LD simulations, namely 2.6 Hz, is in fair agreement with experiment. A comparison to the X-ray structure of the R-isomer shows that the conformation of the crystalline compound occupies the low energy region most highly populated as a single R-conformer (30%) during the LD simulations.     

Solution structure of the d(T-C-G-A) duplex at acidic pH. A parallel-stranded helix containing C+ .C, G.G and A.A pairs

The solution structure of the d(T-C-G-A) sequence at acidic pH has been determined by a combination of NMR and molecular dynamics calculations including NOE intensity based refinements. This sequence forms a right-handed parallel-stranded duplex with C+ .C (three hydrogen bonds along Watson-Crick edge), G.G (two symmetry related N2-H.. N3 hydrogen bonds) and A.A (two symmetry related N6-H..N7 hydrogen bonds) homo base-pair formation at acidic pH. The duplex is stabilized by intra-strand base stacking at the C2-G3 step and cross-strand base stacking at the G3-A4 step. The thymine residues on partner strands are directed towards each other and are positioned over the C+ .C base-pair. All four residues adopt anti glycosidic torsion angles and C2'-endo type sugar conformations in the parallel-stranded d(T-C-G-A) duplex which exhibits large changes in twist angles between adjacent steps along the duplex. This study rules out previously proposed models for the structure of the d(T-C-G-A) duplex at acidic pH and supports earlier structural contributions, which established that d(C-G) and d(C-G-A) containing sequences at acidic pH pair through parallel-stranded alignment. We have also monitored hydration patterns in the symmetry related grooves of the parallel-stranded d(T-C-G-A) duplex.     

Disallowed Ramachandran conformations of amino acid residues in protein structures

An analysis of the nature and distribution of disallowed Ramachandran conformations of amino acid residues observed in high resolution protein crystal structures has been carried out. A data set consisting of 110 high resolution, non-homologous, protein crystal structures from the Brookhaven Protein Data Bank was examined. The data set consisted of a total of 18,708 non-Gly residues, which were characterized on the basis of their backbone dihedral angles (phi, psi). Residues falling outside the defined "broad allowed limits" on the Ramachandran map were chosen and the reported B-factor value of the alpha-carbon atom was used to further select well defined disallowed conformations. The conformations of the selected 66 disallowed residues clustered in distinct regions of the Ramachandran map indicating that specific phi, psi angle distortions are preferred under compulsions imposed by local constraints. The distribution of various amino acid residues in the disallowed residue data set showed a predominance of small polar/charged residues, with bulky hydrophobic residues being infrequent. As a further check, for all the 66 cases non-hydrogen van der Waals short contacts in the protein structures were evaluated and compared with the ideal "Ala-dipeptide" constructed using disallowed dihedral angle (phi, psi) values. The analysis reveals that short contacts are eliminated in most cases by local distortions of bond angles. An analysis of the conformation of the identified disallowed residues in related protein structures reveals instances of conservation of unusual stereochemistry.     

Crystalline and molecular structure of the K+-complex of meso-valinomycin, cyclo(-(D-Val-L-Hyi-L-Val-D-Hyi)3-).KAuCl4

Crystal structure of the complex of meso-valinomycin with KAuCl4 (C60H102N6O18KAuCl4) was determined using direct X-ray diffraction analysis. The conformational state of the complex is similar to that determined earlier for free meso-valinomycin. Characteristic of it is the centrosymmetric bracelet shape stabilized by six intramolecular NH...OC hydrogen bonds of 4 --> 1 type. The K+ ion is located in an inner negatively charged octahedral cavity formed by six carbonyl oxygen atoms of ester groups. The observed differences in conformational angles of the complex and free are caused by readjustment of the geometry of the ion-binding cavity to the size of the ion bound during complexation.     

Helix-forming tendencies of amino acids depend on their sequence contexts: tripeptides AFG and FAG show incipient beta-bulge formation in their crystal structures

Many of the theoretical methods used for predicting the occurrence of alpha-helices in peptides are based on the helical preferences of amino acid monomer residues. In order to check whether the helix-forming tendencies are based on helical preferences of monomers only or also on their sequence contexts, we synthesized permuted sequences of the tripeptides GAF, GAV, and GAL that formed crystalline helices with near alpha-helical conformation. The tripeptides AFG and FAG formed good crystals. The x-ray crystallographic studies of AFG and FAG showed that though they contain the same amino acids as GAF but in different sequences, they do not assume a helical conformation in the solid state. On the other hand, AFG and FAG, which contain the same amino acids but in a different sequence, exhibit nearly the same backbone torsion angles corresponding to an incipient formation of a beta-bulge, and exhibit nearly identical unit cells and crystal structures. Based on these results, it appears that the helix-forming tendencies of amino acids depend on the sequence context in which it occurs in a polypeptide. The synthetic peptides AFG (L-Ala-L-Phe-Gly) and FAG (L-Phe-L-Ala-Gly), C14H19N3O4, crystallize in the orthorhombic space group P2(1)2(1)2(1), with a = 5.232(1), b = 14.622(2), c = 19.157(3) A, Dx = 1.329 g cm-3, Z = 4, R = 0.041 for 549 reflections for AFG, and with a = 5.488(2), b = 14.189(1), c = 18.562(1) A, Dx = 1.348 g cm-3, Z = 4, R = 0.038 for 919 reflections for FAG. Unlike the other tripeptides GAF, GGV, GAL, and GAI, the crystals of AFG and FAG do not contain water molecule, and the molecules of AFG aor FAG do not show the helical conformation. The torsion angles at the backbone of the peptide are psi 1 = 144.5(5) degrees; phi 2, psi 2 = -98.1(6) degrees, -65.2(6) degrees; phi 3, psi 13, psi 31 = 154.1(6) degrees, -173.6(6) degrees, 6.9(8) degrees for AFG; and psi 1 = 162.6(3) degrees; phi 2, psi 2 = -96.7(4) degrees, -46.3(4) degrees; phi 3, psi 13, psi 31 = 150.1(3) degrees, -168.7(3) degrees, 12.2(5) degrees for FAG. The conformation angles (phi, psi) for residues 2 and 3 for both AFG and FAG show incipient formation of an beta-bulge.     

Main-chain conformational features at different conformations of the side-chains in proteins

An analysis of the known protein structures has shown that the main-chain torsion angles, phi and psi of a residue can be affected by the side-chain torsion angle, chi1. The (chi1, psi) plot of all residues (except Gly, Ala and Pro) show six distinct regions where points are concentrated-although some of these regions are nearly absent in specific cases. The mean of these clusters can show a shift along the psi axis by as much as 30 degrees as chi1 is changed from around 180 to -60 to 60 degrees. Because of the lesser steric constraint points are more diffused along the psi axis when chi1 is approximately -60 degrees. Although points are more spread out along the phi axis in the (chi1, phi) plot, the dependence of phi on chi1 shows up in a shortened phi range (by about 30 degrees) when chi1 is around -60 degrees, and a distinct tendency of clustering of points into two regions when chi1 is approximately equal to 60 degrees, especially for the aromatic residues. Based on the dependence of the backbone conformation on its side-chain the 17 amino acids can be grouped into five classes: (i) aliphatic residues branched at the Cbeta position (although Thr is atypical), (ii) Leu (branched at the Cgamma position), (iii) aromatic residues (Trp can show some deviations), (iv) short polar residues (Asp and Asn), and (v) the remaining linear-chain residues, mainly polar. Ser and Thr have the highest inclination to occur with two different orientations of the side-chain that can be located through crystallography. Such residues exhibiting two chi1 angles have their phi and psi angles in a region that is common to the Ramachandran plots at the two different chi1 angles. The dependence of phi and psi angles on chi1 can be used to understand the helical propensities of some residues. Moreover, the average phi, psi values in the alpha-helices vary with the side-chain conformation.     

Trisaccharide synthesis by glycosyl transfer from p-nitrophenyl beta-D-N-acetylgalactosaminide on to disaccharide acceptors catalysed by the beta-N-acetylhexosaminidase from Aspergillus oryzae

The beta-N-acetylhexosaminidase from Aspergillus oryzae catalysed the transfer of beta-D-N-acetylgalactosaminyl residues from p-nitrophenyl beta-D-N-acetylglucosaminide on to disaccharide acceptors consisting of thioethyl glycosides of alpha-D-Glc-(1-->4)-beta-D-Glc, beta-D-Glc-(1-->4)-beta-D-Glc and beta-D-Glc-(1-->6)-beta-D-Glc. The principle of 'anomeric control' was exemplified by the results which showed that an alpha-linkage between the units of the acceptor favoured exclusively the formation of a new (1-->4)-linkage, whereas the beta-configuration in the acceptor led to a mixture of (1-->4)- and (1-->3)-linked products, as observed for simple glycosides of monosaccharide acceptors. With the thioethyl beta-lactoside as acceptor, beta-D-Gal-(1-->6)-beta-D-Gal-(1-->4)-beta-D-GlcSEt was formed, owing to the action of residual beta-D-galactosidase activity in the N-acetylhexosaminidase on the thioethyl beta-lactoside acting as both donor and acceptor.