Abstract

The trisaccharide beta-D-Glcp-(1-->2)-beta-D-Glcp-(1-->3)-alpha-D-Glcp-OMe has been investigated by molecular dynamics (MD) simulations and NMR experiments in water. 13C spin-lattice (T1) and spin-spin (T2) relaxation times, together with 1H,13C NOE data were measured at two magnetic field strengths (9.4 and 14.1 T) in a 277 K D2O solution. Relaxation data interpreted by means of the model-free formalism revealed a rigid (S2 approximately 0.9) oligosaccharide tumbling in solution. 1H,1H Cross-relaxation rates were determined at 600 MHz by 1D DPFGSE NOESY and T-ROESY experiments, which provided high quality data and subsequently proton-proton distances within the trisaccharide. The presence of anti conformers at both torsions of a glycosidic linkage is demonstrated for the first time. MD simulations were carried out to facilitate analysis of the NOE data. In total, 15 simulations-starting from five different conformational states--were performed, with production runs of up to 10 ns, resulting in 83 ns of oligosaccharide dynamics in water. anti Conformers were populated to different degrees in the simulations, especially at the phi2 torsion angle. By combining the results from the NOE experiments and the MD simulations, the anti conformers at the (1-->2)-linkage were quantified as 7% anti-phi2 and 2% anti-psi2, revealing a highly flexible trisaccharide in which large conformational changes occur. From the MD simulations, interresidue hydrogen bonding, from HO2" to O2 or O3, was significantly populated (approximately 40%) in both of the anti conformational states. The contentious issue over rigidity versus flexibility in oligosaccharides has thus been thoroughly examined, showing that the dynamics should be taken into account for a relevant description of the molecular system.

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