Published in

Elsevier, Carbohydrate Research, 1(284), p. 35-49

DOI: 10.1016/0008-6215(96)00013-4

Links

Tools

Export citation

Search in Google Scholar

Molecular structure of [4-(4-cyanobenzoyl) phenyl] 1,5-dithio-β-D-xylopyranoside (naroparcil) in the solid state and in solution: An investigation by X-ray crystallography, molecular mechanics calculations, and NMR spectroscopy

This paper is available in a repository.
This paper is available in a repository.

Full text: Download

Green circle
Preprint: archiving allowed
Red circle
Postprint: archiving forbidden
Red circle
Published version: archiving forbidden
Data provided by SHERPA/RoMEO

Abstract

The conformational behavior of a representative of a new class of oral venous antithrombotic agents, [4-(4-cyanobenzoyl) phenyl] 1,5-dithio-β-d-xylopyranoside (naroparcil) (1) has been characterized by X-ray crystallography, molecular modeling and NMR studies. The crystal structure of 1 belongs to the monoclinic space group P21, with two independent molecules in the asymmetric unit. The unit cell has dimensions of a = 11.641, , and β = 102.29°. The present work provides structural information on the influence of substitution of intracyclic and glycosidic oxygen atoms by sulfur atoms, as well as on the influence of aromatic rings on the carbohydrate moiety. The xylopyranoside ring has the classical 4C1 conformation. As for the orientations of the phenyl substituent with respect to the xylopyranose the values observed in the two independent molecules are strikingly different (-85°, -177°) and (-102°, 144°). The 1H-1H NOE across the glycosidic bond has been measured by NOESY experiments. In parallel, a conformational analysis using the crystal coordinates as the starting point has been made using the Tripos force field. The resulting potential energy surface indicates a high flexibility about the glycosidic linkage. The theoretical NMR data were calculated taking into account all the accessible conformations and using the averaging methods appropriate for slow internal motions. The agreement between experimental and theoretical data is excellent and constitutes a satisfactory test of the validity of the conformational energy surface.