A conformational dynamics study of alpha-l-Rhap-(1-->2)[alpha-l-Rhap-(1-->3)]-alpha-l-Rhap-OMe in solution by NMR experiments and molecular simulations.

The conformational preference of alpha-l-Rhap-(1-->2)[alpha-l-Rhap-(1-->3)]-alpha-l-Rhap-OMe in solution has been studied by NMR spectroscopy using one-dimensional (1)H,(1)H T-ROESY experiments and measurement of trans-glycosidic (3)J(C,H) coupling constants. Molecular dynamics (MD) simulations with a CHARMM22 type of force field modified for carbohydrates were performed with water as the explicit solvent. The homonuclear cross-relaxation rates, interpreted as effective proton-proton distances, were compared to those obtained from simulation. Via a Karplus torsional relationship, (3)J(C,H) values were calculated from simulation and compared to experimental data. Good agreement was observed between experimental data and the MD simulation, except for one inter-residue T-ROE between protons in the terminal sugar residues. The results show that the trisaccharide exhibits substantial conformational flexibility, in particular along the psi glycosidic torsion angles. Notably, for these torsions, a high degree of correlation (77%) was observed in the MD simulation revealing either psi(2)(+) psi(3)(+) or psi(2)(-)psi(3)(-) states. The simulations also showed that non-exoanomeric conformations were present at the phi torsion angles, but to a limited extent, with the phi(3) state populated to a larger extent than the phi(2) state. Further NMR analysis of the trisaccharide by translational diffusion measurements and (13)C T(1) relaxation experiments quantified global reorientation using an anisotropic model together with interpretation of the internal dynamics via the "model-free" approach. Fitting of the dynamically averaged states to experimental data showed that the psi(2)(+)psi(3)(+) state is present to approximately 49%, psi(2)(-) psi(3)(-) to approximately 39%, and phi(3) (non-exo) to approximately 12%. Finally, using a dynamic and population-averaged model, (1)H,(1)H T-ROE buildup curves were calculated using a full relaxation matrix approach and were found to be in excellent agreement with experimental data, in particular for the above inter-residue proton-proton interaction between the terminal residues.

Structural analysis of the O-antigen polysaccharide from Escherichia coli O152.

The structure of the O-antigen polysaccharide (PS) from Escherichia coli O152 has been determined. Component analysis together with 1H, 13C and 31P NMR spectroscopy were used to elucidate the structure. Inter-residue correlations were determined by 1H,31P COSY, 1H,1H NOESY and 1H,13C heteronuclear multiple-bond correlation experiments. The PS is composed of pentasaccharide repeating units with the following structure: [structure: see text]. The structure is similar to that of the O-antigen polysaccharide from E. coli O173. The cross-reactivity between E. coli O152 and E. coli O3 may be explained by structural similarities in the branching region of their O-antigen polysaccharides.

NMR and molecular modeling studies of the interaction between wheat germ agglutinin and the beta-D-GlcpNAc-(1-->6)-alpha-D-Manp epitope present in glycoproteins of tumor cells.

The beta-D-GlcpNAc-(1-->6)-alpha-D-Manp disaccharide is a constituent of highly branched cell-surface glycoconjugates that are malignancy markers. The conformational preference of the disaccharide beta-D-GlcpNAc-(1-->6)-alpha-D-Manp-OMe in solution has been studied by molecular modeling and NMR spectroscopy including 1D (1)H,(1)H T-ROESY experiments and analysis of (3)J(H,H) of the hydroxymethyl group being part of the glycosidic linkage of the disaccharide, which revealed the relative populations of the omega torsion angle as gt = 0.60, gg = 0.35, and tg = 0.05. Good agreement was obtained between the effective proton-proton distances from the experiment and those obtained by molecular modeling when the flexibility at the omega torsion angle was taken into account. Molecular modeling of the disaccharide in the binding sites of the lectin wheat germ agglutinin indicates that several conformations could be adopted in the bound state. (1)H NMR and transfer NOESY experiments confirmed that binding took place, and trans-glycosidic proton-proton interactions indicated that a conformational preference was present in the bound state, as observed by the relative change of the NOEs from H1' to H6(pro-R) and H6(pro-S). STD NMR experiments showed that binding occurred in the region of the N-acetyl group of the terminal sugar residue. In addition, the O-methyl group received saturation transfer because of the proximity to the protein. (1)H,(1)H NOEs indicated that the two methyl groups were close in space, as observed in only one of the predicted bound conformations. Experimental and theoretical data therefore agree that one conformation with a gt conformation of the hydroxymethyl group and a negative sign for the psi torsion angle is indeed selected by the lectin upon binding.

Dynamics of the Escherichia coli O91 O-antigen polysaccharide in solution as studied by carbon-13 NMR relaxation.

The dynamics of the O-antigen part of the lipopolysaccharide from the enterohemorrhagic Escherichia coli O91 has been determined in solution using (13)C NMR relaxation measurements at two magnetic field strengths, 9.4 and 14.1 T, thereby facilitating the testing of several dynamical models. The biological repeating unit, consisting of five sugar residues and substituents, could be determined by spectral analysis of different (1)H,(13)C correlations and corroborated by the relaxation data. The site specifically (13)C-labeled material was shown to have approximately 10 repeating units with a narrow distribution. A model-free analysis of the relaxation data revealed a complex dynamical behavior where the sugar residues could be described by a global correlation time (tau(m) = 5.4 ns), generalized order parameters (S(2) approximately 0.63), and different correlation times for internal motions related to their position in the repeating unit along the polymer (tau(e) approximately 360-520 ps). One of the sugar residues showed, in addition, a chemical exchange contribution. Furthermore, a substituent on another sugar residue was described by two order parameters (S(f)(2) = 0.51 and S(s)(2) = 0.21). The solution dynamics of the polysaccharide are thus described by highly intricate motions, both in amplitude and time scales. These results are of significance in the general description of polysaccharides surrounding bacterial cell surfaces and in the presentation of antigenic epitopes to the immune system of an invaded host.

A conformational study of alpha-D-Manp-(1-->2)-alpha-D-Manp-(1-->O)-L-Ser by NMR 1H,1H T-ROESY experiments and molecular-dynamics simulations.

The conformational preference of alpha-D-Manp-(1-->2)-alpha-D-Manp-(1-->O)-L-Ser has been investigated by one-dimensional (1)H,(1)H T-ROESY experiments and molecular-dynamics simulations with CHARMM22 type of force fields and water as explicit solvent. Proton-proton distances were obtained from the simulations and subsequently experimentally determined distances could be derived. Measurements were performed on the title compound as well as on selectively deuterium-substituted analogues synthesized as part of this study to alleviate possible NMR spectroscopic difficulties. A very good agreement was present between the separate NMR experiments. In the subsequent analysis a key nuclear Overhauser effect between the anomeric protons in the two sugar residues was used to assess the conformational dynamics revealed by the molecular simulations. The combined results support a model in which two states are significantly populated as a result of flexibility around the bond defined by the glycosidic torsion angle psi.