For complex oligosaccharides, which are relatively rigid with modest excursions from a single minimum energy conformation, it is straightforward to build conformational models from NOE data. Other oligosaccharides are more flexible with transitions between distinct minima separated by substantial energy barriers. We show that modeling based on scalar coupling data is superior to NOE-based modeling for the latter case. Long range 13 C-13 C and 13 C-1 H coupling constants measured for the heptasaccharide repeating subunit of the cell wall polysaccharide from Streptococcus mitis J22 are correlated with individual glycosidic dihedral angles, effectively uncoupling the degrees of freedom of the oligosaccharide and allowing a search for combinations of dihedral angles which are energetically reasonable, i.e., with no bad van der Waals contacts, and which can be combined to satisfy all the measured J values. Allowed values of the individual angles can then be combined to search for overall oligosaccharide conformations which contribute to the ensemble. We show that while the polysaccharide from S. mitis J22 is flexible, requiring multiple conformations, most of the flexibility is localized to a few bonds and only a rather small number of conformations is required to reproduce the experimental NOE and scalar coupling data.A central question in the conformation and dynamics of complex oligosaccharides and polysaccharides is whether a given structure is "flexible" (1-3). In fact, no oligosaccharide is likely to be truly rigid since puckering of the pyranoside ring and fluctuations of the glycosidic dihedral angles must occur to some extent in all cases. But the currently available data allows for classification of the types of internal motion in oligosaccharides into two distinct types. We will identify internal motion of the first kind as rapid motion on a picosecond time scale of the internal degrees of freedom within a local minimum with limited excursions of the dihedral angles. Oligosaccharides exhibiting this type of internal motion are sometimes called "rigid" in the sense that experimental NOE 1 data may agree with that calculated for a model having a single conformation. The blood group oligosaccharides, especially the Lewis type, are probably the best example of a relatively rigid conformation exhibiting primarily internal motion of the first kind (4-9).In addition to this first kind of motion, more flexible oligosaccharides can also present a second kind of internal motion which is characterized by larger excursions of glycosidic dihedral angles crossing high-energy barriers from one well-defined minimum to another. The existence of this second kind of flexibility may be inferred when the experimental data are not compatible with a single conformation. The time scale of such motions depends on the height of the barrier separating the energy minima and could range from nanoseconds to microseconds. At this point, we have available limited information, either experimental or theoretical, regarding the ki...