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The title compound, C16H24O10·0.11H2O, is a key inter­mediate in the synthesis of 2-de­oxy-2-[18F]fluoro-D-glucose (18F-FDG), which is the most widely used mol­ecular-imaging probe for positron emission tomography (PET). The crystal structure has two independent mol­ecules (A and B) in the asymmetric unit, with closely comparable geometries. The pyran­ose ring adopts a 4C1 conformation [Cremer–Pople puckering parameters: Q = 0.553 (2) Å, θ = 16.2 (2)° and φ = 290.4 (8)° for mol­ecule A, and Q = 0.529 (2) Å, θ =15.3 (3)° and φ = 268.2 (9)° for mol­ecule B], and the dioxolane ring adopts an envelope conformation. The chiral centre in the dioxolane ring, introduced during the synthesis of the compound, has an R configuration, with the eth­oxy group exo to the manno­pyran­ose ring. The asymmetric unit also contains one water mol­ecule with a refined site-occupancy factor of 0.222 (8), which bridges between mol­ecules A and B via O—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270112032076/bi3042sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270112032076/bi3042Isup2.hkl
Contains datablock I

CCDC reference: 869277

Comment top

To date, 2-deoxy-2-[18F]fluoro-D-glucose (18F-FDG) [(III); see scheme] has been the most widely used molecular-imaging probe in positron emission tomography (PET) (Alavi & Reivich, 2002; Nutt, 2002). Due to its structural similarity to glucose, 18F-FDG is used to measure the cellular uptake and metabolic rates of local glucose in physiological or pathophysiological conditions. Nowadays, 18F-FDG-PET is used not only in research laboratories to address questions of scientific interest, but also in hospitals as a routine clinical diagnostic tool in cardiology, neurology and oncology (Gambhir et al., 2001).

The title compound, (I), is one of the key intermediates during the synthesis of 18F-FDG (Fig. 2). Hydrolysis of the 1,2-orthoacetate groups of (I) with 1M aqueous HCl, followed by triflation with Tf2O-pyridine (Tf is trifluoromethanesulfonate?), yields 1,3,4,6-tetra-O-acetyl-2-O-trifluoromethanesulfonyl-β-D-mannopyranose (mannose trifluoromethanesulfonate), (II). Nucleophilic [18F] fluorination and acidic/basic deprotection of (II) then provides 18F-FDG, (III) (see scheme) (Toyokuni et al., 2004). Although hydrolysis of (I) gives the desired 1,3,4,6-tetra-O-acetyl-β-D-mannopyranose product, the reaction also produces an undesired 2,3,4,6-tetra-O-acetyl-β-D-mannopyranose by-product, and the yield of the desired reaction is as low as 25–30%. The study of the three-dimensional structure of (I) can help us to understand not only its chemical properties but also the mechanism of the hydrolysis reaction.

The crystal structure of (I) has two independment molecules in the asymmetric unit (molecules A and B; Fig. 1) and a water molecule with a refined site-occupancy factor of 0.222 (8). In molecule A, the C—C bonds within the pyranose ring have bond lengths ranging between 1.510 (3) and 1.523 (3) Å, in accordance with those in a survey of 27 pyranoid rings reported by Arnott & Scott (1972). The exocyclic C1—O1 bond length of 1.398 (3) Å is the shortest in the pyranose ring. The C1—O5 and C5—O5 bond lengths are 1.422 (3) and 1.437 (2) Å, respectively, indicating that C1—O1 is equatorial. The bond angles at the C atoms of the ring vary between 107.28 (15) and 114.27 (17)°, with the angles at C1 and C2 larger than the expected values of 109.2 and 110.5°, respectively, and the angle at C5 smaller than the expected 110.0°. Although the O5—C1—O1 angle [106.47 (18)°] appears normal for equatorial C1—O1, the C5—O5—C1 angle [113.45 (17)°] is somewhat larger than the expected 112.0°. These data indicate that C1—O1 is distorted from an idealized equatorial orientation and is bisectional. This could be explained by the presence of the ethoxyethylidene group at the 1,2-positions. The pyranose ring of molecule B exhibits similar structural features to that of molecule A.

The endocyclic torsion angles in the pyranose rings vary from 40.2 (3) to 65.3 (2)° (absolute values), indicating that the six-membered rings are distorted from an idealized 4C1 chair conformation. The conformation in (I) is different from the skew conformation (3S5) reported for 3,4,6-tri-O-acetyl-l,2-O-[1-(exo-ethoxy)ethylidene]-α-D-glucopyranose (Heitmann et al., 1974). Further insight into the distortions is obtained from the Cremer–Pople puckering parameters (Cremer & Pople, 1975): for molecule A, Q = 0.553 (2) Å, θ = 16.2 (2)° and ϕ = 290.4 (8)°; for molecule B, Q = 0.529 (2) Å, θ = 15.3 (3)° and ϕ = 268.2 (9)°. The extent of the ring distortion, embodied in the value of θ, is slightly greater for molecule A than for molecule B. The direction of the ring distortion, embodied in the value of ϕ, shows a distortion towards a BC2,C5 conformation for molecule A and C1SC5 for molecule B (Jeffrey & Yates, 1979).

In the five-membered ring of molecule A, the C2—O2—C7—O1 torsion angle [5.2 (2)°] indicates an approximately planar structure for these four atoms (r.m.s. deviation from the mean plane = 0.023 Å). Atom C1 deviates from the mean plane by 0.53 Å. In molecule B, the corresponding values are 3.3 (2)°, r.m.s. deviation = 0.015 Å and deviation of C1' = 0.53Å. Thus, the conformation of the dioxolane ring is an envelope, with Cremer–Pople parameters of Q = 0.3486 (21) Å and ϕ = 43.2 (3)° for molecule A, and Q = 0.3392 (21) Å and ϕ = 40.7 (4)° for molecule B.

The bond lengths and angles in the acetoxy groups and acetoxymethyl substituent all appear normal, although the bond angles at C6 [107.47 (16)°] and C6' [107.26 (18)°] are, respectively, 4.3 and 4.5° smaller than the average bond angle (111.8°) found in 23 other pyranose derivatives (Arnott & Scott, 1972). The three substituents all adopt the same equatorial orientation as on the parent compound β-D-mannose, due to the 4C1 conformation of the mannopyranose ring. Similar to what is observed for many acetylated sugars, the acetyl groups directly connected to the sugar ring [i.e. C(ring)—O—C(O)] are close to coplanar with the H atom bound to the same ring C atom (Haines & Hughes, 2007). The O5—C5—C6—O6 [-71.0 (2)°] and O5'—C5'—C6'—O6' [-63.2 (2)°] torsion angles indicate a gg arrangement of the exocyclic C6—O6 (C6'—O6') bond (i.e. H5 anti to O6, and H5' anti to O6').

There are some structural differences on the O1 (O1') and O2 (O2') sides of the five-membered dioxolane ring. In molecule A, the C1—O1 bond [1.398 (3) Å] is the shortest of the four C—O bonds involving O1 and O2, and the other three bonds are almost identical in length [average 1.435 (2) Å]. The O1—C7—C8 angle [113.10 (18)°] is larger than O2—C7—C8 [110.08 (18)°] and the O1—C7—O9 angle [108.90 (17)°] is smaller than O2—C7—O9 [112.19 (17)°]. The C7—O9 bond [1.380 (3) Å] is the shortest of the three ether bonds at C7, with the C7—O1 and C7—O2 bonds effectively identical [average 1.435 (2) Å]. The same structural features are found in molecule B. This might give an indication of why hydrolysis of (I) yields almost equivalent amounts of the two major isomeric products (Toyokuni et al., 2004).

Atom C7 (C7') is the only new chiral centre formed in the synthesis of (I) (Toyokuni et al., 2004). It has an R configuration, with the ethoxy group exo to the mannopyranose ring. The 1H NMR spectrum (CDCl3) gives a single peak at 1.75 p.p.m. for the C8 methyl group, consistent with the conclusion of earlier PMR [proton magnetic resonance? Is this not the same as 1H NMR?] studies of glucopyranose 1,2-(alkyl orthoacetates) (Lemieux & Morgan, 1965), namely that the diastereomer for which the C8 methyl H atoms resonate at a lower field has the configuration in which the alkoxy group is exo to the pyranose ring.

The bicyclic ring structure of (I) has five pendant groups, each of which terminates in a methyl group. In the packing of the crystal structure, the pendant groups of one molecule lie between pendant groups from other molecules (Fig. 2). The partially occupied water molecules bridge between molecules A and B, forming hydrogen bonds (Table 1). Thermogravimetric analysis was carried out for (I), but it is difficult to detect any water loss prior to decomposition of the compound, since the solvent water accounts for only approximately 0.52% of the mass.

Related literature top

For related literature, see: Alavi & Reivich (2002); Arnott & Scott (1972); Cremer & Pople (1975); Gambhir et al. (2001); Haines & Hughes (2007); Heitmann et al. (1974); Jeffrey & Yates (1979); Lemieux & Morgan (1965); Nutt (2002); Toyokuni et al. (2004).

Experimental top

The title compound was synthesized according to the literature procedure of Toyokuni et al. (2004). The crude product was recrystallized from ethanol (m.p. 375.0–375.8 K; literature value 374–376 K). Spectroscopic analysis: 1H NMR (400 MHz, CDCl3, δ, p.p.m.): 1.18 (t, J = 7.1 Hz, 3H, MeCH2O), 1.75 (s, 3H, MeCO2), 2.05 (s, 3H, Ac), 2.07 (s, 3H, Ac), 2.12 (s, 3H, Ac), 3.56 (m, 2H, MeCH2O), 3.68 (ddd, J = 9.5, 4.9 and 2.7 Hz, 1H, H5), 4.14 (dd, J = 12.1 and 2.6 Hz, 1H) and 4.24 (dd, J = 12.1 and 4.9 Hz, 1H, 2 H6), 4.60 (dd, J = 3.9 and 2.7 Hz, 1H, H2), 5.15 (dd, J = 9.9 and 4.0 Hz, 1H, H3), 5.30 (t, J = 9.7 Hz, 1H, H4), 5.48 (d, J = 2.5 Hz, 1H, H1).

Refinement top

All H atoms bound to C atoms were placed geometrically and refined using a riding model, with C—H = 0.98–1.00 Å and Uiso(H) = 1.2Ueq(C). The H atoms of the water molecule were placed so as to form hydrogen bonds to atoms O62 and O62', with O—H = 0.85 Å, then refined as riding with Uiso(H) = 1.2Ueq(O). In the absence of significant anomalous scattering, the absolute structure could not be determined. Friedel pairs were not merged. The absolute structure is assigned on the basis of nonchanging chiral centres in the synthetic procedure (Toyokuni et al., 2004).

Computing details top

Data collection: CrystalClear (Rigaku, 2008); cell refinement: CrystalClear (Rigaku, 2008); data reduction: CrystalClear (Rigaku, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of (I), showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.
[Figure 2] Fig. 2. The molecular packing of (I), viewed along the a axis. Dashed lines indicate hydrogen bonds.
3,4,6-Tri-O-acetyl-1,2-O-[1-(exo-ethoxy)ethylidene]- β-D-mannopyranose 0.11-hydrate top
Crystal data top
C16H24O10·0.11H2OF(000) = 804.1
Mr = 378.35Dx = 1.336 Mg m3
Monoclinic, P21Melting point: 375(1) K
Hall symbol: P 2ybMo Kα radiation, λ = 0.71073 Å
a = 5.6353 (14) ÅCell parameters from 6897 reflections
b = 30.987 (8) Åθ = 1.9–29.1°
c = 10.817 (3) ŵ = 0.11 mm1
β = 95.232 (4)°T = 153 K
V = 1881.0 (8) Å3Prism, colourless
Z = 40.48 × 0.16 × 0.09 mm
Data collection top
Rigaku AFC10/Saturn724+ CCD area-detector
diffractometer
9788 independent reflections
Radiation source: Rotating Anode7008 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
Detector resolution: 28.5714 pixels mm-1θmax = 29.1°, θmin = 2.0°
ϕ and ω scansh = 77
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
k = 4242
Tmin = 0.948, Tmax = 0.990l = 1410
16933 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.092H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0286P)2 + 0.126P]
where P = (Fo2 + 2Fc2)/3
9788 reflections(Δ/σ)max = 0.001
491 parametersΔρmax = 0.28 e Å3
1 restraintΔρmin = 0.25 e Å3
Crystal data top
C16H24O10·0.11H2OV = 1881.0 (8) Å3
Mr = 378.35Z = 4
Monoclinic, P21Mo Kα radiation
a = 5.6353 (14) ŵ = 0.11 mm1
b = 30.987 (8) ÅT = 153 K
c = 10.817 (3) Å0.48 × 0.16 × 0.09 mm
β = 95.232 (4)°
Data collection top
Rigaku AFC10/Saturn724+ CCD area-detector
diffractometer
9788 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
7008 reflections with I > 2σ(I)
Tmin = 0.948, Tmax = 0.990Rint = 0.031
16933 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0481 restraint
wR(F2) = 0.092H-atom parameters constrained
S = 1.00Δρmax = 0.28 e Å3
9788 reflectionsΔρmin = 0.25 e Å3
491 parameters
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R-factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O50.8636 (2)0.45959 (5)0.04398 (14)0.0312 (3)
O10.6685 (2)0.42257 (5)0.11403 (14)0.0347 (4)
O20.3815 (2)0.47107 (5)0.07284 (14)0.0303 (3)
O90.2780 (2)0.40593 (5)0.17216 (14)0.0337 (4)
O30.3927 (2)0.55907 (5)0.04668 (14)0.0309 (3)
O320.5734 (3)0.62239 (6)0.07937 (19)0.0531 (5)
O40.7865 (2)0.56936 (4)0.15016 (14)0.0313 (3)
O420.4739 (3)0.57101 (6)0.2636 (2)0.0684 (6)
O60.8605 (3)0.48057 (5)0.30227 (15)0.0397 (4)
O621.0778 (4)0.50142 (9)0.4712 (2)0.0903 (9)
C10.7817 (4)0.46184 (7)0.0841 (2)0.0325 (5)
H10.91590.46720.13660.039*
C20.5820 (3)0.49448 (7)0.1110 (2)0.0294 (5)
H20.55850.50030.20220.035*
C30.6191 (3)0.53655 (7)0.0408 (2)0.0288 (5)
H30.73620.55460.08190.035*
C40.7130 (4)0.52882 (7)0.0928 (2)0.0283 (5)
H40.58850.51480.13930.034*
C50.9350 (4)0.50064 (7)0.0967 (2)0.0307 (5)
H51.05410.51430.04580.037*
C61.0480 (4)0.49292 (8)0.2268 (2)0.0313 (5)
H6A1.16860.46970.22670.038*
H6B1.12760.51950.26010.038*
C70.4279 (4)0.42573 (7)0.0812 (2)0.0321 (5)
C80.3915 (4)0.40412 (8)0.0393 (2)0.0348 (5)
H8A0.42690.37330.03320.042*
H8B0.22570.40790.05770.042*
H8C0.49800.41710.10580.042*
C100.2872 (4)0.42123 (9)0.2971 (2)0.0423 (6)
H10A0.44710.41610.32520.051*
H10B0.25330.45260.30180.051*
C110.1007 (4)0.39646 (9)0.3769 (2)0.0491 (7)
H11A0.05740.40310.35080.059*
H11B0.13150.36540.36780.059*
H11C0.10660.40480.46400.059*
C310.3969 (4)0.60271 (7)0.0619 (2)0.0319 (5)
C320.1558 (4)0.62116 (8)0.0537 (2)0.0409 (6)
H32A0.16420.65270.05800.049*
H32B0.09660.61260.02500.049*
H32C0.04750.61040.12290.049*
C410.6559 (4)0.58621 (8)0.2366 (2)0.0383 (6)
C420.7745 (5)0.62599 (9)0.2896 (3)0.0535 (7)
H42A0.68380.63740.35550.064*
H42B0.78080.64770.22410.064*
H42C0.93680.61900.32420.064*
C610.8929 (4)0.48938 (9)0.4234 (2)0.0430 (6)
C620.6754 (5)0.47921 (10)0.4860 (3)0.0571 (7)
H62A0.54590.49860.45510.069*
H62B0.70880.48310.57590.069*
H62C0.62810.44920.46840.069*
O5'0.7257 (3)0.72173 (5)0.46258 (14)0.0349 (4)
O1'0.5646 (2)0.75239 (5)0.28572 (13)0.0326 (4)
O2'0.2849 (2)0.77158 (5)0.41517 (13)0.0309 (3)
O9'0.1856 (3)0.76709 (5)0.20215 (13)0.0341 (4)
O3'0.3304 (3)0.80834 (5)0.65264 (14)0.0320 (3)
O32'0.4834 (3)0.87446 (5)0.63163 (19)0.0527 (5)
O4'0.6280 (3)0.74569 (5)0.78283 (14)0.0352 (4)
O42'0.2669 (3)0.71985 (6)0.81867 (16)0.0476 (4)
O6'0.6093 (3)0.65333 (5)0.60743 (14)0.0373 (4)
O62'0.8014 (3)0.59298 (6)0.6711 (2)0.0654 (6)
C1'0.6854 (4)0.76166 (7)0.4009 (2)0.0329 (5)
H1'0.83820.77730.39190.039*
C2'0.5078 (4)0.79017 (7)0.4616 (2)0.0314 (5)
H2'0.51850.82050.43110.038*
C3'0.5357 (4)0.78950 (7)0.6017 (2)0.0305 (5)
H3'0.68000.80670.63110.037*
C4'0.5674 (4)0.74414 (7)0.65092 (19)0.0297 (5)
H4'0.41890.72690.63080.036*
C5'0.7769 (4)0.72340 (8)0.5946 (2)0.0335 (5)
H5'0.92280.74130.61520.040*
C6'0.8262 (4)0.67786 (8)0.6370 (2)0.0406 (6)
H6C0.95800.66550.59390.049*
H6D0.87220.67720.72750.049*
C7'0.3158 (4)0.74908 (7)0.3021 (2)0.0306 (5)
C8'0.2340 (4)0.70305 (7)0.3113 (2)0.0360 (5)
H8D0.26380.68750.23540.043*
H8E0.06310.70250.32170.043*
H8F0.32190.68910.38290.043*
C10'0.2347 (4)0.81131 (8)0.1738 (2)0.0414 (6)
H10C0.40380.81480.15770.050*
H10D0.20240.83020.24410.050*
C11'0.0741 (5)0.82293 (9)0.0600 (3)0.0558 (7)
H11D0.09240.81870.07650.067*
H11E0.11070.80450.00930.067*
H11F0.09930.85320.03850.067*
C31'0.3278 (4)0.85167 (8)0.6655 (2)0.0344 (5)
C32'0.1114 (4)0.86636 (8)0.7227 (2)0.0383 (6)
H32D0.02310.86810.65870.046*
H32E0.14090.89490.76030.046*
H32F0.07380.84580.78690.046*
C41'0.4646 (4)0.73065 (8)0.8572 (2)0.0360 (5)
C42'0.5647 (5)0.72956 (9)0.9888 (2)0.0511 (7)
H42D0.67380.70501.00180.061*
H42E0.43490.72651.04260.061*
H42F0.65140.75641.00910.061*
C61'0.6220 (4)0.61080 (8)0.6300 (2)0.0420 (6)
C62'0.3890 (5)0.58903 (8)0.5965 (3)0.0502 (7)
H62D0.39460.55960.62980.060*
H62E0.35760.58800.50590.060*
H62F0.26170.60520.63160.060*
O211.0055 (16)0.5179 (3)0.7203 (9)0.056 (4)0.222 (8)
H21A1.03530.50990.64810.067*0.222 (8)
H21B0.93790.54240.71420.067*0.222 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O50.0249 (7)0.0284 (8)0.0399 (9)0.0014 (6)0.0010 (7)0.0050 (7)
O10.0227 (7)0.0346 (9)0.0470 (10)0.0010 (7)0.0045 (7)0.0137 (8)
O20.0205 (7)0.0285 (8)0.0426 (9)0.0018 (6)0.0061 (6)0.0058 (7)
O90.0290 (8)0.0342 (9)0.0374 (9)0.0035 (7)0.0001 (7)0.0089 (7)
O30.0217 (7)0.0269 (8)0.0448 (9)0.0004 (6)0.0068 (6)0.0018 (7)
O320.0298 (9)0.0391 (10)0.0924 (15)0.0003 (8)0.0156 (9)0.0164 (10)
O40.0271 (7)0.0281 (8)0.0398 (9)0.0074 (6)0.0089 (6)0.0082 (7)
O420.0584 (12)0.0652 (14)0.0891 (15)0.0256 (11)0.0477 (11)0.0381 (12)
O60.0335 (8)0.0475 (10)0.0385 (9)0.0102 (8)0.0055 (7)0.0027 (8)
O620.0718 (15)0.150 (3)0.0503 (13)0.0474 (16)0.0138 (11)0.0256 (14)
C10.0220 (10)0.0372 (13)0.0391 (13)0.0030 (9)0.0071 (9)0.0085 (10)
C20.0211 (10)0.0329 (12)0.0343 (12)0.0012 (9)0.0037 (9)0.0042 (10)
C30.0173 (9)0.0317 (12)0.0379 (12)0.0032 (9)0.0059 (9)0.0025 (10)
C40.0232 (10)0.0276 (11)0.0350 (12)0.0038 (9)0.0073 (9)0.0049 (9)
C50.0235 (10)0.0314 (12)0.0379 (13)0.0071 (9)0.0068 (9)0.0050 (10)
C60.0214 (10)0.0378 (13)0.0344 (12)0.0027 (9)0.0016 (9)0.0011 (10)
C70.0245 (11)0.0291 (11)0.0423 (13)0.0021 (9)0.0011 (10)0.0083 (10)
C80.0301 (11)0.0345 (13)0.0399 (13)0.0013 (10)0.0037 (10)0.0039 (11)
C100.0424 (14)0.0510 (16)0.0337 (13)0.0057 (12)0.0043 (11)0.0052 (12)
C110.0517 (15)0.0523 (17)0.0417 (15)0.0008 (13)0.0037 (12)0.0106 (13)
C310.0265 (11)0.0300 (12)0.0394 (13)0.0028 (9)0.0047 (9)0.0046 (10)
C320.0282 (11)0.0331 (13)0.0619 (16)0.0004 (10)0.0076 (11)0.0096 (12)
C410.0375 (13)0.0366 (13)0.0422 (14)0.0066 (11)0.0108 (11)0.0090 (11)
C420.0563 (17)0.0431 (15)0.0621 (18)0.0082 (13)0.0105 (14)0.0182 (14)
C610.0406 (14)0.0454 (15)0.0443 (15)0.0006 (12)0.0102 (12)0.0044 (12)
C620.0546 (16)0.0625 (19)0.0573 (17)0.0104 (14)0.0216 (14)0.0103 (14)
O5'0.0301 (8)0.0384 (9)0.0367 (9)0.0047 (7)0.0047 (7)0.0031 (7)
O1'0.0236 (7)0.0427 (9)0.0325 (8)0.0017 (7)0.0078 (6)0.0032 (7)
O2'0.0221 (7)0.0389 (9)0.0324 (8)0.0031 (6)0.0071 (6)0.0055 (7)
O9'0.0323 (8)0.0333 (8)0.0361 (9)0.0035 (7)0.0005 (7)0.0011 (7)
O3'0.0304 (8)0.0288 (8)0.0381 (9)0.0001 (7)0.0093 (7)0.0060 (7)
O32'0.0489 (10)0.0318 (10)0.0796 (14)0.0052 (8)0.0183 (10)0.0051 (9)
O4'0.0342 (8)0.0405 (9)0.0306 (8)0.0022 (7)0.0016 (7)0.0056 (7)
O42'0.0410 (10)0.0550 (11)0.0470 (10)0.0104 (9)0.0057 (8)0.0089 (9)
O6'0.0359 (9)0.0348 (9)0.0402 (9)0.0054 (7)0.0013 (7)0.0005 (7)
O62'0.0569 (12)0.0533 (13)0.0837 (15)0.0252 (10)0.0064 (11)0.0010 (11)
C1'0.0261 (11)0.0362 (12)0.0370 (12)0.0020 (10)0.0070 (9)0.0018 (10)
C2'0.0230 (10)0.0343 (12)0.0376 (13)0.0034 (9)0.0064 (9)0.0026 (10)
C3'0.0233 (10)0.0314 (11)0.0374 (13)0.0008 (9)0.0057 (9)0.0063 (10)
C4'0.0266 (10)0.0334 (12)0.0289 (11)0.0014 (9)0.0018 (9)0.0061 (9)
C5'0.0259 (11)0.0399 (13)0.0341 (12)0.0003 (10)0.0004 (9)0.0046 (11)
C6'0.0313 (12)0.0443 (15)0.0452 (15)0.0063 (11)0.0027 (11)0.0085 (12)
C7'0.0240 (10)0.0340 (12)0.0343 (12)0.0002 (9)0.0049 (9)0.0021 (10)
C8'0.0333 (12)0.0336 (12)0.0424 (14)0.0035 (10)0.0103 (11)0.0040 (10)
C10'0.0409 (14)0.0338 (13)0.0492 (15)0.0025 (11)0.0024 (12)0.0006 (11)
C11'0.0634 (18)0.0413 (16)0.0603 (19)0.0018 (14)0.0086 (15)0.0080 (14)
C31'0.0358 (13)0.0322 (12)0.0341 (13)0.0001 (10)0.0026 (10)0.0040 (10)
C32'0.0381 (13)0.0374 (13)0.0389 (14)0.0076 (11)0.0006 (11)0.0047 (11)
C41'0.0462 (14)0.0287 (12)0.0340 (12)0.0020 (11)0.0080 (11)0.0026 (10)
C42'0.0688 (19)0.0472 (16)0.0367 (14)0.0058 (14)0.0013 (13)0.0019 (13)
C61'0.0479 (15)0.0376 (14)0.0413 (14)0.0142 (12)0.0090 (12)0.0025 (11)
C62'0.0541 (16)0.0362 (14)0.0608 (18)0.0011 (12)0.0075 (14)0.0007 (13)
O210.076 (7)0.040 (6)0.051 (6)0.001 (5)0.001 (4)0.009 (4)
Geometric parameters (Å, º) top
O5—C11.422 (3)O5'—C5'1.432 (3)
O5—C51.437 (2)O1'—C1'1.394 (3)
O1—C11.398 (3)O1'—C7'1.433 (2)
O1—C71.436 (2)O2'—C2'1.431 (2)
O2—C71.434 (3)O2'—C7'1.432 (2)
O2—C21.435 (2)O9'—C7'1.369 (3)
O9—C71.380 (3)O9'—C10'1.437 (3)
O9—C101.437 (3)O3'—C31'1.350 (3)
O3—C311.363 (3)O3'—C3'1.449 (2)
O3—C31.451 (2)O32'—C31'1.208 (3)
O32—C311.196 (2)O4'—C41'1.359 (3)
O4—C411.347 (3)O4'—C4'1.437 (2)
O4—C41.445 (2)O42'—C41'1.201 (3)
O42—C411.189 (3)O6'—C61'1.341 (3)
O6—C611.335 (3)O6'—C6'1.450 (3)
O6—C61.445 (2)O62'—C61'1.201 (3)
O62—C611.180 (3)C1'—C2'1.527 (3)
C1—C21.521 (3)C1'—H1'1.0000
C1—H11.0000C2'—C3'1.509 (3)
C2—C31.514 (3)C2'—H2'1.0000
C2—H21.0000C3'—C4'1.508 (3)
C3—C41.512 (3)C3'—H3'1.0000
C3—H31.0000C4'—C5'1.520 (3)
C4—C51.523 (3)C4'—H4'1.0000
C4—H41.0000C5'—C6'1.502 (3)
C5—C61.510 (3)C5'—H5'1.0000
C5—H51.0000C6'—H6C0.9900
C6—H6A0.9900C6'—H6D0.9900
C6—H6B0.9900C7'—C8'1.505 (3)
C7—C81.496 (3)C8'—H8D0.9800
C8—H8A0.9800C8'—H8E0.9800
C8—H8B0.9800C8'—H8F0.9800
C8—H8C0.9800C10'—C11'1.504 (3)
C10—C111.508 (3)C10'—H10C0.9900
C10—H10A0.9900C10'—H10D0.9900
C10—H10B0.9900C11'—H11D0.9800
C11—H11A0.9800C11'—H11E0.9800
C11—H11B0.9800C11'—H11F0.9800
C11—H11C0.9800C31'—C32'1.489 (3)
C31—C321.484 (3)C32'—H32D0.9800
C32—H32A0.9800C32'—H32E0.9800
C32—H32B0.9800C32'—H32F0.9800
C32—H32C0.9800C41'—C42'1.484 (3)
C41—C421.492 (3)C42'—H42D0.9800
C42—H42A0.9800C42'—H42E0.9800
C42—H42B0.9800C42'—H42F0.9800
C42—H42C0.9800C61'—C62'1.491 (4)
C61—C621.487 (3)C62'—H62D0.9800
C62—H62A0.9800C62'—H62E0.9800
C62—H62B0.9800C62'—H62F0.9800
C62—H62C0.9800O21—H21A0.8500
O5'—C1'1.414 (3)O21—H21B0.8501
C1—O5—C5113.45 (17)C1'—O1'—C7'107.91 (16)
C1—O1—C7107.76 (15)C2'—O2'—C7'108.95 (15)
C7—O2—C2108.93 (15)C7'—O9'—C10'117.25 (17)
C7—O9—C10116.79 (18)C31'—O3'—C3'117.15 (17)
C31—O3—C3117.23 (16)C41'—O4'—C4'117.62 (17)
C41—O4—C4118.80 (17)C61'—O6'—C6'116.43 (19)
C61—O6—C6117.32 (17)O1'—C1'—O5'106.59 (17)
O1—C1—O5106.47 (18)O1'—C1'—C2'102.58 (17)
O1—C1—C2102.74 (16)O5'—C1'—C2'112.74 (18)
O5—C1—C2112.81 (17)O1'—C1'—H1'111.5
O1—C1—H1111.5O5'—C1'—H1'111.5
O5—C1—H1111.5C2'—C1'—H1'111.5
C2—C1—H1111.5O2'—C2'—C3'110.78 (17)
O2—C2—C3111.52 (17)O2'—C2'—C1'101.82 (17)
O2—C2—C1101.36 (17)C3'—C2'—C1'114.29 (18)
C3—C2—C1114.27 (17)O2'—C2'—H2'109.9
O2—C2—H2109.8C3'—C2'—H2'109.9
C3—C2—H2109.8C1'—C2'—H2'109.9
C1—C2—H2109.8O3'—C3'—C4'108.32 (17)
O3—C3—C4110.38 (16)O3'—C3'—C2'111.26 (17)
O3—C3—C2108.17 (15)C4'—C3'—C2'111.43 (18)
C4—C3—C2111.32 (18)O3'—C3'—H3'108.6
O3—C3—H3109.0C4'—C3'—H3'108.6
C4—C3—H3109.0C2'—C3'—H3'108.6
C2—C3—H3109.0O4'—C4'—C3'109.21 (17)
O4—C4—C3109.54 (17)O4'—C4'—C5'106.81 (16)
O4—C4—C5106.50 (15)C3'—C4'—C5'108.91 (18)
C3—C4—C5109.44 (16)O4'—C4'—H4'110.6
O4—C4—H4110.4C3'—C4'—H4'110.6
C3—C4—H4110.4C5'—C4'—H4'110.6
C5—C4—H4110.4O5'—C5'—C6'106.59 (18)
O5—C5—C6108.00 (17)O5'—C5'—C4'108.75 (17)
O5—C5—C4107.28 (15)C6'—C5'—C4'113.8 (2)
C6—C5—C4113.12 (18)O5'—C5'—H5'109.2
O5—C5—H5109.5C6'—C5'—H5'109.2
C6—C5—H5109.5C4'—C5'—H5'109.2
C4—C5—H5109.5O6'—C6'—C5'107.26 (18)
O6—C6—C5107.47 (16)O6'—C6'—H6C110.3
O6—C6—H6A110.2C5'—C6'—H6C110.3
C5—C6—H6A110.2O6'—C6'—H6D110.3
O6—C6—H6B110.2C5'—C6'—H6D110.3
C5—C6—H6B110.2H6C—C6'—H6D108.5
H6A—C6—H6B108.5O9'—C7'—O2'112.21 (17)
O9—C7—O2112.19 (17)O9'—C7'—O1'109.43 (17)
O9—C7—O1108.90 (17)O2'—C7'—O1'105.51 (16)
O2—C7—O1105.31 (16)O9'—C7'—C8'107.06 (18)
O9—C7—C8107.35 (18)O2'—C7'—C8'110.07 (18)
O2—C7—C8110.08 (18)O1'—C7'—C8'112.65 (18)
O1—C7—C8113.10 (18)C7'—C8'—H8D109.5
C7—C8—H8A109.5C7'—C8'—H8E109.5
C7—C8—H8B109.5H8D—C8'—H8E109.5
H8A—C8—H8B109.5C7'—C8'—H8F109.5
C7—C8—H8C109.5H8D—C8'—H8F109.5
H8A—C8—H8C109.5H8E—C8'—H8F109.5
H8B—C8—H8C109.5O9'—C10'—C11'106.86 (19)
O9—C10—C11106.7 (2)O9'—C10'—H10C110.4
O9—C10—H10A110.4C11'—C10'—H10C110.4
C11—C10—H10A110.4O9'—C10'—H10D110.4
O9—C10—H10B110.4C11'—C10'—H10D110.4
C11—C10—H10B110.4H10C—C10'—H10D108.6
H10A—C10—H10B108.6C10'—C11'—H11D109.5
C10—C11—H11A109.5C10'—C11'—H11E109.5
C10—C11—H11B109.5H11D—C11'—H11E109.5
H11A—C11—H11B109.5C10'—C11'—H11F109.5
C10—C11—H11C109.5H11D—C11'—H11F109.5
H11A—C11—H11C109.5H11E—C11'—H11F109.5
H11B—C11—H11C109.5O32'—C31'—O3'122.3 (2)
O32—C31—O3123.3 (2)O32'—C31'—C32'126.3 (2)
O32—C31—C32126.3 (2)O3'—C31'—C32'111.3 (2)
O3—C31—C32110.41 (18)C31'—C32'—H32D109.5
C31—C32—H32A109.5C31'—C32'—H32E109.5
C31—C32—H32B109.5H32D—C32'—H32E109.5
H32A—C32—H32B109.5C31'—C32'—H32F109.5
C31—C32—H32C109.5H32D—C32'—H32F109.5
H32A—C32—H32C109.5H32E—C32'—H32F109.5
H32B—C32—H32C109.5O42'—C41'—O4'123.2 (2)
O42—C41—O4123.7 (2)O42'—C41'—C42'125.9 (2)
O42—C41—C42126.8 (2)O4'—C41'—C42'110.9 (2)
O4—C41—C42109.5 (2)C41'—C42'—H42D109.5
C41—C42—H42A109.5C41'—C42'—H42E109.5
C41—C42—H42B109.5H42D—C42'—H42E109.5
H42A—C42—H42B109.5C41'—C42'—H42F109.5
C41—C42—H42C109.5H42D—C42'—H42F109.5
H42A—C42—H42C109.5H42E—C42'—H42F109.5
H42B—C42—H42C109.5O62'—C61'—O6'123.3 (2)
O62—C61—O6122.1 (2)O62'—C61'—C62'125.1 (3)
O62—C61—C62126.8 (3)O6'—C61'—C62'111.7 (2)
O6—C61—C62111.0 (2)C61'—C62'—H62D109.5
C61—C62—H62A109.5C61'—C62'—H62E109.5
C61—C62—H62B109.5H62D—C62'—H62E109.5
H62A—C62—H62B109.5C61'—C62'—H62F109.5
C61—C62—H62C109.5H62D—C62'—H62F109.5
H62A—C62—H62C109.5H62E—C62'—H62F109.5
H62B—C62—H62C109.5H21A—O21—H21B108.1
C1'—O5'—C5'116.61 (17)
C7—O1—C1—O584.09 (19)C7'—O1'—C1'—O5'84.20 (19)
C7—O1—C1—C234.7 (2)C7'—O1'—C1'—C2'34.5 (2)
C5—O5—C1—O1166.39 (15)C5'—O5'—C1'—O1'160.68 (15)
C5—O5—C1—C254.4 (2)C5'—O5'—C1'—C2'48.9 (2)
C7—O2—C2—C3147.16 (17)C7'—O2'—C2'—C3'145.17 (18)
C7—O2—C2—C125.2 (2)C7'—O2'—C2'—C1'23.2 (2)
O1—C1—C2—O236.21 (19)O1'—C1'—C2'—O2'35.0 (2)
O5—C1—C2—O278.0 (2)O5'—C1'—C2'—O2'79.3 (2)
O1—C1—C2—C3156.28 (17)O1'—C1'—C2'—C3'154.44 (17)
O5—C1—C2—C342.1 (2)O5'—C1'—C2'—C3'40.2 (3)
C31—O3—C3—C497.2 (2)C31'—O3'—C3'—C4'152.51 (18)
C31—O3—C3—C2140.77 (19)C31'—O3'—C3'—C2'84.7 (2)
O2—C2—C3—O349.7 (2)O2'—C2'—C3'—O3'51.8 (2)
C1—C2—C3—O3163.94 (17)C1'—C2'—C3'—O3'166.11 (18)
O2—C2—C3—C471.7 (2)O2'—C2'—C3'—C4'69.2 (2)
C1—C2—C3—C442.5 (2)C1'—C2'—C3'—C4'45.1 (2)
C41—O4—C4—C3109.4 (2)C41'—O4'—C4'—C3'111.8 (2)
C41—O4—C4—C5132.3 (2)C41'—O4'—C4'—C5'130.5 (2)
O3—C3—C4—O470.19 (19)O3'—C3'—C4'—O4'65.7 (2)
C2—C3—C4—O4169.67 (16)C2'—C3'—C4'—O4'171.59 (16)
O3—C3—C4—C5173.39 (16)O3'—C3'—C4'—C5'177.99 (16)
C2—C3—C4—C553.3 (2)C2'—C3'—C4'—C5'55.3 (2)
C1—O5—C5—C6172.48 (16)C1'—O5'—C5'—C6'176.82 (17)
C1—O5—C5—C465.3 (2)C1'—O5'—C5'—C4'60.1 (2)
O4—C4—C5—O5178.00 (16)O4'—C4'—C5'—O5'179.19 (17)
C3—C4—C5—O563.7 (2)C3'—C4'—C5'—O5'61.4 (2)
O4—C4—C5—C659.0 (2)O4'—C4'—C5'—C6'62.2 (2)
C3—C4—C5—C6177.33 (18)C3'—C4'—C5'—C6'180.00 (18)
C61—O6—C6—C5152.7 (2)C61'—O6'—C6'—C5'175.28 (19)
O5—C5—C6—O671.0 (2)O5'—C5'—C6'—O6'63.2 (2)
C4—C5—C6—O647.6 (2)C4'—C5'—C6'—O6'56.7 (2)
C10—O9—C7—O260.1 (2)C10'—O9'—C7'—O2'59.8 (2)
C10—O9—C7—O156.0 (2)C10'—O9'—C7'—O1'57.0 (2)
C10—O9—C7—C8178.82 (18)C10'—O9'—C7'—C8'179.35 (18)
C2—O2—C7—O9113.11 (19)C2'—O2'—C7'—O9'115.75 (18)
C2—O2—C7—O15.2 (2)C2'—O2'—C7'—O1'3.3 (2)
C2—O2—C7—C8127.43 (18)C2'—O2'—C7'—C8'125.14 (19)
C1—O1—C7—O9139.93 (18)C1'—O1'—C7'—O9'141.51 (18)
C1—O1—C7—O219.4 (2)C1'—O1'—C7'—O2'20.6 (2)
C1—O1—C7—C8100.8 (2)C1'—O1'—C7'—C8'99.5 (2)
C7—O9—C10—C11177.13 (18)C7'—O9'—C10'—C11'178.8 (2)
C3—O3—C31—O325.6 (3)C3'—O3'—C31'—O32'3.1 (3)
C3—O3—C31—C32174.50 (18)C3'—O3'—C31'—C32'178.02 (17)
C4—O4—C41—O424.8 (4)C4'—O4'—C41'—O42'6.7 (3)
C4—O4—C41—C42175.65 (19)C4'—O4'—C41'—C42'173.17 (19)
C6—O6—C61—O629.9 (4)C6'—O6'—C61'—O62'0.8 (4)
C6—O6—C61—C62173.8 (2)C6'—O6'—C61'—C62'179.8 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O21—H21A···O620.851.972.808 (10)170
O21—H21B···O620.851.792.629 (9)169

Experimental details

Crystal data
Chemical formulaC16H24O10·0.11H2O
Mr378.35
Crystal system, space groupMonoclinic, P21
Temperature (K)153
a, b, c (Å)5.6353 (14), 30.987 (8), 10.817 (3)
β (°) 95.232 (4)
V3)1881.0 (8)
Z4
Radiation typeMo Kα
µ (mm1)0.11
Crystal size (mm)0.48 × 0.16 × 0.09
Data collection
DiffractometerRigaku AFC10/Saturn724+ CCD area-detector
diffractometer
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.948, 0.990
No. of measured, independent and
observed [I > 2σ(I)] reflections
16933, 9788, 7008
Rint0.031
(sin θ/λ)max1)0.684
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.048, 0.092, 1.00
No. of reflections9788
No. of parameters491
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.28, 0.25

Computer programs: CrystalClear (Rigaku, 2008), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), DIAMOND (Brandenburg, 1999).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O21—H21A···O620.851.972.808 (10)169.7
O21—H21B···O62'0.851.792.629 (9)169.4
 

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