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The relative configuration of the title compound, C8H14O6, was firmly established by X-ray crystallographic analysis. The absolute configuration was determined by the use of 2-C-methyl-D-ribono-1,4-lactone as the starting material. The crystal structure is stabilized by O—H...O hydrogen bonds, with each mol­ecule acting as a donor and an acceptor for five hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807030541/lh2443sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807030541/lh2443Isup2.hkl
Contains datablock I

CCDC reference: 657698

Key indicators

  • Single-crystal X-ray study
  • T = 150 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.024
  • wR factor = 0.059
  • Data-to-parameter ratio = 9.3

checkCIF/PLATON results

No syntax errors found



Alert level C ABSTM02_ALERT_3_C The ratio of expected to reported Tmax/Tmin(RR') is < 0.90 Tmin and Tmax reported: 0.810 0.990 Tmin(prime) and Tmax expected: 0.964 0.988 RR(prime) = 0.839 Please check that your absorption correction is appropriate. PLAT061_ALERT_3_C Tmax/Tmin Range Test RR' too Large ............. 0.84
Alert level G REFLT03_ALERT_4_G Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF. From the CIF: _diffrn_reflns_theta_max 27.51 From the CIF: _reflns_number_total 1185 Count of symmetry unique reflns 1213 Completeness (_total/calc) 97.69% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no PLAT791_ALERT_1_G Confirm the Absolute Configuration of C1 = . R PLAT791_ALERT_1_G Confirm the Absolute Configuration of C2 = . R PLAT791_ALERT_1_G Confirm the Absolute Configuration of C5 = . R PLAT791_ALERT_1_G Confirm the Absolute Configuration of C6 = . R PLAT860_ALERT_3_G Note: Number of Least-Squares Restraints ....... 1
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 6 ALERT level G = General alerts; check 4 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Carbohydrates are one of the most varied cheap chiral building blocks (Lichtenthaler & Peters, 2004) available. Currently, there are very limited examples of di-branched carbohydrates reported. Examples of sugars that contain two carbon branches in the literature include 2,4-dimethyl-3,4-O-isopropylidene-L-arabinono-1,5-lactone (Booth et al. 2007a) and various protected forms of 3,5-Di-C-methyl-mannono and glucono lactone (Booth, Watkin et al., 2007; Booth et al., 2007a,b,c).

The Kiliani ascension on ketoses and deoxy ketoses has proved a valuable route towards branched sugars (Hotchkiss et al. 2004;2006, Soengas et al., 2005, Jones, Watkin et al. 2007). Branched sugars still remains a relatively unstudied class of compounds but recent biological results have indicated they could have a potential use as therapeutics (Mitchell et al. 2007).

The crystal structure of the title compound (Fig. 1) exists as a three-dimensionally hydrogen bonded lattice with each molecule acting as a donor and an acceptor for 5 hydrogen bonds. One of the hydrogen bonds, from O8—H11, is bifurcated (Fig. 2).

Related literature top

For related literature, see: Jones, Curran et al. (2007); Jones, Watkin et al. (2007); Mitchell et al. (2007); Hotchkiss et al. (2006, 2004); Soengas et al. (2005).

For related literature, see: Booth et al. (2007, 2007a, 2007b, 2007c); Görbitz (1999); Lichtenthaler & Peters (2004).

Experimental top

Treatment of 1-deoxy-3-C-methyl-D-psicose 1 (see Fig. 3) (Jones, Curran et al. 2007) derived from 2-C-methyl-D-ribono-1,4-lactone (Hotchkiss et al., 2006), with sodium cyanide, gave a mixture of 2,6-anhydro derivative 2 and lactone 3 Deprotection of lactone 3 gave an equilibrium of 1,5-lactone 4 and 1,4-lactone 5 in which 2,3-C-dimethyl-D-allono-lactone exists as 2,3-C-dimethyl-D-allono-1,4-lactone 5 in the crystalline state. X-Ray crystallographic analysis shows that the structure is the title compound 5 removing ambiguities as to the stereochemistry at the new C-2 chiral centre. The title compound was crystallized from a mixture of cyclohexane and ethyl acetate; m.p. 426–428 K; [α]D22 +66.8 (c, 0.65 in methanol).

Refinement top

In the absence of significant anomalous scattering, Friedel pairs were merged and the absolute configuration was assigned by the starting material.

The relatively large ratio of minimum to maximum corrections applied in the multiscan process (1:1.22) reflect changes in the illuminated volume of the crystal. Changes in illuminated volume were kept to a minimum, and were taken into account (Görbitz, 1999) by the multi-scan inter-frame scaling (DENZO/SCALEPACK, Otwinowski & Minor, 1997).

The H atoms were all located in a difference map, but those attached to carbon atoms were repositioned geometrically. The H atoms were initially refined with soft restraints on the bond lengths and angles to regularize their geometry (C—H in the range 0.93–0.98, O—H = 0.82 Å) and Uiso(H) (in the range 1.2–1.5 times Ueq of the parent atom), after which the positions were refined with riding constraints.

Structure description top

Carbohydrates are one of the most varied cheap chiral building blocks (Lichtenthaler & Peters, 2004) available. Currently, there are very limited examples of di-branched carbohydrates reported. Examples of sugars that contain two carbon branches in the literature include 2,4-dimethyl-3,4-O-isopropylidene-L-arabinono-1,5-lactone (Booth et al. 2007a) and various protected forms of 3,5-Di-C-methyl-mannono and glucono lactone (Booth, Watkin et al., 2007; Booth et al., 2007a,b,c).

The Kiliani ascension on ketoses and deoxy ketoses has proved a valuable route towards branched sugars (Hotchkiss et al. 2004;2006, Soengas et al., 2005, Jones, Watkin et al. 2007). Branched sugars still remains a relatively unstudied class of compounds but recent biological results have indicated they could have a potential use as therapeutics (Mitchell et al. 2007).

The crystal structure of the title compound (Fig. 1) exists as a three-dimensionally hydrogen bonded lattice with each molecule acting as a donor and an acceptor for 5 hydrogen bonds. One of the hydrogen bonds, from O8—H11, is bifurcated (Fig. 2).

For related literature, see: Jones, Curran et al. (2007); Jones, Watkin et al. (2007); Mitchell et al. (2007); Hotchkiss et al. (2006, 2004); Soengas et al. (2005).

For related literature, see: Booth et al. (2007, 2007a, 2007b, 2007c); Görbitz (1999); Lichtenthaler & Peters (2004).

Computing details top

Data collection: COLLECT (Nonius, 2001); cell refinement: DENZO/SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO/SCALEPACK; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: CAMERON (Watkin et al., 1996); software used to prepare material for publication: CRYSTALS.

Figures top
[Figure 1] Fig. 1. The title compound with displacement ellipsoids drawn at the 50% probability level. H atoms are shown as spheres of arbitary radius.
[Figure 2] Fig. 2. Packing diagram showing the title compound projected along the a-axis.
[Figure 3] Fig. 3. The reaction scheme.
2,3-C-Dimethyl-D-allono-1,4-lactone top
Crystal data top
C8H14O6F(000) = 220
Mr = 206.20Dx = 1.398 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 1103 reflections
a = 6.1387 (2) Åθ = 5–27°
b = 7.4088 (3) ŵ = 0.12 mm1
c = 10.8142 (3) ÅT = 150 K
β = 94.996 (2)°Plate, colourless
V = 489.97 (3) Å30.30 × 0.20 × 0.10 mm
Z = 2
Data collection top
Nonius KappaCCD
diffractometer
1151 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.022
ω scansθmax = 27.5°, θmin = 5.5°
Absorption correction: multi-scan
(DENZO/SCALEPACK; Otwinowski & Minor, 1997)
h = 77
Tmin = 0.81, Tmax = 0.99k = 98
4427 measured reflectionsl = 1413
1185 independent reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.024H-atom parameters constrained
wR(F2) = 0.059 w = 1/[σ2(F2) + 0.11P],
where P = [max(Fo2,0) + 2Fc2]/3
S = 0.98(Δ/σ)max = 0.000341
1185 reflectionsΔρmax = 0.22 e Å3
127 parametersΔρmin = 0.15 e Å3
1 restraint
Crystal data top
C8H14O6V = 489.97 (3) Å3
Mr = 206.20Z = 2
Monoclinic, P21Mo Kα radiation
a = 6.1387 (2) ŵ = 0.12 mm1
b = 7.4088 (3) ÅT = 150 K
c = 10.8142 (3) Å0.30 × 0.20 × 0.10 mm
β = 94.996 (2)°
Data collection top
Nonius KappaCCD
diffractometer
1185 independent reflections
Absorption correction: multi-scan
(DENZO/SCALEPACK; Otwinowski & Minor, 1997)
1151 reflections with I > 2σ(I)
Tmin = 0.81, Tmax = 0.99Rint = 0.022
4427 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0241 restraint
wR(F2) = 0.059H-atom parameters constrained
S = 0.98Δρmax = 0.22 e Å3
1185 reflectionsΔρmin = 0.15 e Å3
127 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.8416 (2)0.4263 (2)0.78654 (13)0.0150
C20.7563 (2)0.3296 (2)0.66461 (13)0.0162
C30.6629 (2)0.4883 (2)0.58761 (13)0.0167
O40.60598 (17)0.62177 (17)0.66215 (9)0.0191
C50.6621 (2)0.5717 (2)0.79221 (12)0.0142
C60.7150 (2)0.7452 (2)0.86458 (13)0.0167
C70.5125 (2)0.8654 (2)0.86070 (13)0.0183
O80.55256 (18)1.02775 (17)0.92964 (10)0.0217
O90.79185 (17)0.69964 (18)0.98862 (9)0.0202
O100.63373 (19)0.49872 (19)0.47585 (9)0.0248
O110.57031 (17)0.22808 (17)0.69455 (9)0.0201
C120.9154 (3)0.2152 (3)0.60015 (15)0.0271
O130.83413 (16)0.30793 (17)0.88832 (9)0.0184
C141.0685 (2)0.5052 (2)0.77945 (14)0.0213
H510.53130.51080.82090.0186*
H610.83240.81050.82550.0186*
H710.40190.79620.90000.0210*
H720.46470.89080.77340.0213*
H1210.83510.16080.52710.0417*
H1220.97370.12260.65700.0412*
H1231.03180.28990.57170.0413*
H1411.11070.56860.85660.0333*
H1421.17130.41010.76920.0338*
H1431.06150.58630.70910.0340*
H40.68130.64401.01710.0323*
H100.96440.28520.92450.0307*
H110.61691.09780.88490.0359*
H140.50630.17480.63200.0313*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0152 (6)0.0146 (7)0.0149 (6)0.0006 (6)0.0000 (5)0.0030 (5)
C20.0178 (7)0.0149 (7)0.0159 (6)0.0015 (6)0.0015 (5)0.0011 (5)
C30.0181 (7)0.0155 (7)0.0163 (6)0.0009 (6)0.0004 (5)0.0002 (6)
O40.0258 (5)0.0159 (5)0.0145 (5)0.0043 (4)0.0041 (4)0.0000 (4)
C50.0155 (6)0.0141 (7)0.0124 (6)0.0003 (5)0.0023 (5)0.0007 (5)
C60.0180 (6)0.0155 (7)0.0163 (6)0.0042 (6)0.0004 (5)0.0007 (6)
C70.0238 (7)0.0128 (7)0.0181 (6)0.0004 (6)0.0012 (5)0.0017 (6)
O80.0309 (6)0.0132 (5)0.0220 (5)0.0040 (5)0.0076 (4)0.0024 (4)
O90.0211 (5)0.0222 (6)0.0162 (5)0.0057 (5)0.0046 (4)0.0002 (4)
O100.0349 (6)0.0247 (6)0.0141 (5)0.0031 (5)0.0022 (4)0.0021 (5)
O110.0243 (5)0.0180 (5)0.0176 (5)0.0074 (5)0.0006 (4)0.0012 (4)
C120.0317 (8)0.0262 (9)0.0238 (7)0.0093 (7)0.0051 (6)0.0030 (7)
O130.0171 (5)0.0197 (5)0.0177 (5)0.0014 (4)0.0030 (4)0.0074 (4)
C140.0149 (7)0.0248 (8)0.0240 (7)0.0026 (6)0.0003 (5)0.0029 (7)
Geometric parameters (Å, º) top
C1—C21.5509 (19)C6—H610.992
C1—C51.547 (2)C7—O81.4253 (17)
C1—O131.4110 (17)C7—H710.977
C1—C141.518 (2)C7—H720.982
C2—C31.523 (2)O8—H110.832
C2—O111.4277 (17)O9—H40.873
C2—C121.509 (2)O11—H140.850
C3—O41.3413 (18)C12—H1210.981
C3—O101.2087 (17)C12—H1220.970
O4—C51.4663 (16)C12—H1230.974
C5—C61.5249 (19)O13—H100.876
C5—H510.994C14—H1410.972
C6—C71.527 (2)C14—H1420.958
C6—O91.4232 (17)C14—H1430.968
C2—C1—C599.57 (11)C5—C6—H61108.8
C2—C1—O13110.17 (12)C7—C6—H61108.9
C5—C1—O13109.28 (11)O9—C6—H61108.9
C2—C1—C14112.23 (12)C6—C7—O8112.03 (12)
C5—C1—C14113.17 (13)C6—C7—H71106.1
O13—C1—C14111.78 (11)O8—C7—H71108.0
C1—C2—C3101.06 (12)C6—C7—H72108.2
C1—C2—O11105.55 (10)O8—C7—H72111.4
C3—C2—O11105.10 (11)H71—C7—H72111.0
C1—C2—C12117.88 (13)C7—O8—H11106.9
C3—C2—C12114.12 (12)C6—O9—H4103.9
O11—C2—C12111.80 (14)C2—O11—H14112.8
C2—C3—O4110.23 (11)C2—C12—H121107.6
C2—C3—O10127.72 (14)C2—C12—H122108.8
O4—C3—O10122.01 (14)H121—C12—H122110.6
C3—O4—C5109.77 (11)C2—C12—H123110.4
C1—C5—O4104.29 (10)H121—C12—H123108.1
C1—C5—C6119.14 (12)H122—C12—H123111.2
O4—C5—C6107.52 (11)C1—O13—H10112.2
C1—C5—H51107.1C1—C14—H141108.7
O4—C5—H51106.6C1—C14—H142109.8
C6—C5—H51111.4H141—C14—H142108.9
C5—C6—C7109.92 (11)C1—C14—H143107.5
C5—C6—O9108.80 (11)H141—C14—H143111.4
C7—C6—O9111.49 (11)H142—C14—H143110.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O9—H4···O8i0.871.812.683 (2)178
O13—H10···O9ii0.881.812.675 (2)169
O8—H11···O13iii0.832.052.762 (2)144
O11—H14···O10iv0.851.902.729 (2)163
O8—H11···O11iii0.832.272.954 (2)140
Symmetry codes: (i) x+1, y1/2, z+2; (ii) x+2, y1/2, z+2; (iii) x, y+1, z; (iv) x+1, y1/2, z+1.

Experimental details

Crystal data
Chemical formulaC8H14O6
Mr206.20
Crystal system, space groupMonoclinic, P21
Temperature (K)150
a, b, c (Å)6.1387 (2), 7.4088 (3), 10.8142 (3)
β (°) 94.996 (2)
V3)489.97 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.12
Crystal size (mm)0.30 × 0.20 × 0.10
Data collection
DiffractometerNonius KappaCCD
Absorption correctionMulti-scan
(DENZO/SCALEPACK; Otwinowski & Minor, 1997)
Tmin, Tmax0.81, 0.99
No. of measured, independent and
observed [I > 2σ(I)] reflections
4427, 1185, 1151
Rint0.022
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.059, 0.98
No. of reflections1185
No. of parameters127
No. of restraints1
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.22, 0.15

Computer programs: COLLECT (Nonius, 2001), DENZO/SCALEPACK (Otwinowski & Minor, 1997), DENZO/SCALEPACK, SIR92 (Altomare et al., 1994), CRYSTALS (Betteridge et al., 2003), CAMERON (Watkin et al., 1996), CRYSTALS.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O9—H4···O8i0.871.812.683 (2)178
O13—H10···O9ii0.881.812.675 (2)169
O8—H11···O13iii0.832.052.762 (2)144
O11—H14···O10iv0.851.902.729 (2)163
O8—H11···O11iii0.832.272.954 (2)140
Symmetry codes: (i) x+1, y1/2, z+2; (ii) x+2, y1/2, z+2; (iii) x, y+1, z; (iv) x+1, y1/2, z+1.
 

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