organic compounds
Re®nement
equivalents [3030 for (I) and 560 for (II)] were merged before the
®nal re®nements. The enantiomer used in each model was based on
the known chirality of the precursor sugars, viz. d-glucose and
d-galactose, from which (I) and (II), respectively, were synthesized.
For both compounds, data collection: MSC/AFC Diffractometer
Control Software (Molecular Structure Corporation, 1991); cell
re®nement: MSC/AFC Diffractometer Control Software; data reduc-
tion: TEXSAN (Molecular Structure Corporation, 1999); program(s)
used to solve structure: SHELXS97 (Sheldrick, 1997); program(s)
used to re®ne structure: SHELXL97 (Sheldrick, 1997); molecular
graphics: ORTEPII (Johnson, 1976); software used to prepare
material for publication: SHELXL97 and PLATON (Spek, 2001).
Re®nement on F2
R[F2 > 2ꢅ(F2)] = 0.042
wR(F2) = 0.103
S = 1.03
4302 re¯ections
421 parameters
H atoms treated by a mixture of
independent and constrained
re®nement
w = 1/[ꢅ2(Fo2) + (0.0379P)2
+ 0.5383P]
where P = (Fo2 + 2Fc2)/3
(Á/ꢅ)max = 0.001
Ê ꢂ3
Áꢆmax = 0.21 e A
Ê ꢂ3
Áꢆmin = ꢂ0.22 e A
Extinction correction: SHELXL97
(Sheldrick, 1997)
Extinction coef®cient: 0.0024 (5)
Table 2
Hydrogen-bonding geometry (A, ) for (II).
ꢁ
Ê
DÐHÁ Á ÁA
DÐH
HÁ Á ÁA
DÁ Á ÁA
DÐHÁ Á ÁA
Supplementary data for this paper are available from the IUCr electronic
archives (Reference: GG1083). Services for accessing these data are
described at the back of the journal.
O1ÐH1Á Á ÁO15
0.77 (3)
2.10 (3)
2.765 (3)
145 (3)
References
Examination of the structure of (I) with PLATON (Spek, 2001)
revealed that the unit-cell parameters can be transformed metrically
to an orthorhombic C lattice, but that the overall structure itself is not
consistent with the higher symmetry. For (I), the anisotropic dis-
placement ellipsoids for O16 and, to a lesser extent, O18 are signif-
icantly elongated. In addition, the maximum peak of residual electron
Berman, H. M., Chu, S. S. C. & Jeffrey, G. A. (1967). Science, 157, 1576±1577.
Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew Chem.
Int. Ed. Engl. 34, 1555±1573.
Bichard, C. J. F., Mitchell, E. P., Wormald, M. R., Watson, K. A., Johnson, L. N.,
Zographos, S. E., Koutra, D. D., Oikonomakos, N. G. & Fleet, G. W. J.
(1995). Tetrahedron Lett. 36, 2145±2148.
Cremer, D. & Pople, J. A. (1975). J. Am. Chem. Soc. 97, 1354±1358.
Flack, H. D. (1983). Acta Cryst. A39, 876±881.
Flack, H. D. & Bernardinelli, G. (2000). J. Appl. Cryst. 33, 1143±1148.
Jiang, S., Singh, G. & Wightman, R. H. (1996). Chem. Lett. pp. 67±68.
Johnson, C. K. (1976). ORTEPII. Report ORNL-5138. Oak Ridge National
Laboratory, Tennessee, USA.
Kanters, J. A., Scherrenberg, R. L., Lee¯ang, B. R., Kroon, J. & Mathlouthi, M.
(1988). Carbohydr. Res. 180, 175±182.
Kanters, K. A., Kock, A. J. H. M. & Roelofsen, G. (1978). Acta Cryst. B34,
3285±3288.
Longchambon, F., Ohannessian, J., Avenel, D. & Neuman, A. (1975). Acta
Cryst. B31, 2623±2627.
Martin, J. L., Veluraja, K., Ross, K., Johnson, L. N., Fleet, G. W. J., Ramsden,
N. G., Bruce, I., Orchard, M. G., Oikonomakos, N. G., Papageorgiou, A. C.,
Leonidas, D. D. & Tsitoura, H. S. (1991). Biochemistry, 30, 10101±10116.
Molecular Structure Corporation (1991). MSC/AFC Diffractometer Control
Software. MSC, 3200 Research Forest Drive, The Woodlands, TX 77381,
USA.
Molecular Structure Corporation (1999). TEXSAN. Version 1.10. MSC, 9009
New Trails Drive, The Woodlands, TX 77381±5209, USA.
Pougny, J.-R., Nassr, M. A. M. & SinayÈ, P. (1981). J. Chem. Soc. Chem.
Commun. pp. 375±376.
Ê ꢂ3
Ê
density of 0.49 e A is 1.0 A from O16 and the next highest peak is
Ê ꢂ3
only 0.25 e A . This suggests that these two atoms may be disor-
dered, particularly O16. Indeed, the position of O16 could be divided
Ê
into two almost equally occupied sites that are approximately 0.5 A
apart, and the re®nement of this model reduced R(F) to 0.035 and the
Ê ꢂ3
maximum peak of residual electron density to 0.25 e A . Never-
theless, the anisotropic displacement ellipsoid for one of the disor-
dered positions became even more elongated than that of O16 in the
ordered model, even when light restraints were applied, and more
severe restraints upset the realism of the geometric parameters.
Therefore, it was considered to be more appropriate to use the
ordered model in the ®nal re®nement. For each compound, the
methyl H atoms were constrained to an ideal geometry (CÐH =
Ê
0.98 A) with Uiso(H) = 1.5Ueq(C), but were allowed to rotate freely
about the CÐC bonds. The positions of the hydroxy H atoms were
re®ned freely, along with individual isotropic displacement para-
meters. All other H atoms were placed in geometrically idealized
Ê
positions (CÐH = 0.95±1.00 A) and constrained to ride on their
parent atoms, with Uiso(H) = 1.2Ueq(C). The absolute con®guration
could not be determined because of the absence of signi®cant
anomalous scatterers in the compound, and attempts to con®rm the
absolute structure by re®nement of the Flack parameter (Flack, 1983)
led to inconclusive values (Flack & Bernardinelli, 2000) for this
parameter [ꢂ0.7 (7) for (I) and ꢂ0.3 (11) for (II)]. Therefore, Friedel
È
Sheldrick, G. M. (1997). SHELXL97 and SHELXS97. University of Got-
tingen, Germany.
Shriner, R. L. (1942). Org. React. 1, 1±37.
Spek, A. L. (2001). PLATON. University of Utrecht, The Netherlands.
Watson, K. A., Mitchell, E. P., Johnson, L. N., Son, J. C., Bichard, C. J. F.,
Orchard, M. G., Fleet, G. W. J., Oikonomakos, N. G., Leonidas, D. D., Konyo,
M. & Papageorgiou, A. C. (1994). Biochemistry, 33, 5745±5748.
ꢀ
1420 Linden, Li and Lee
C18H26O12 and C38H42O8
Acta Cryst. (2001). C57, 1418±1420