supplementary materials


Acta Cryst. (2009). E65, o33    [ doi:10.1107/S1600536808040555 ]

2,2,3,3-Tetrafluorobutane-1,4-diol

M. M. Reichvilser, F. W. Roessner and P. Klüfers

Abstract top

In the title compound, C4H6F4O2, a partially fluorinated aliphatic diol, cooperative O-H...O hydrogen bonds form R22(14) rings, which are connected into infinite layers parallel to the (100) plane by C(7) chains. A C-H...F link is also seen.

Comment top

The asymmetric unit of the title compound contains one complete molecule, which is shown in Figure 1.

The molecular packing is dominated by two O—H···O hydrogen bonds. According to graph set theory [Bernstein et al. (1995), Etter et al. (1990)] the descriptors C(7) and R22(14) can be assigned. Together with one C—H···F hydrogen bond [motif C(5)] the first-level (unitary) graph set N1 = C(5)C(7)R22(14) is obtained.

Figure 2 shows a cutout of the layers parallel to the (100) plane which are generated by the O—H···O hydrogen bond framework. The C—H···F bonds which are located within these layers are omitted for clarity.

Due to packing effects and the specific hydrogen bonding interactions the O1—C1—C2—C3—C4—O2 chain adopts a somewhat unusual conformation. The substituents at the C2—C3 fragment are staggered with the CH2OH moieties being gauche to each other. For Newman projections see Fig. 3.

Related literature top

For crystal structures containing 2,2,3,3-tetrafluorobutane-1,4-dioxy units, see: Elias et al. (1994); Beşli et al. (2004, 2005, 2006). For details on graph-set analysis of hydrogen-bond networks, see: Bernstein et al. (1995); Etter et al. (1990).

Experimental top

The title compound was obtained from Acros Organics. A single-crystal suitable for X-ray diffraction was isolated from the supplied material.

Refinement top

All H atoms were found in difference maps. C-bonded H atoms were positioned geometrically (C—H = 0.99 Å) and treated as riding on their parent atoms [Uiso(H) = 1.2Ueq(C)]. Coordinates of O-bonded H atoms and O—H distances were refined freely [Uiso(H) = 1.5Ueq(O)].

Computing details top

Data collection: COLLECT (Hooft, 2004); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK and DENZO (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, with atom labels and anisotropic displacement ellipsoids (drawn at 50% probability level) for non-H atoms.
[Figure 2] Fig. 2. Hydrogen bonding in (I). [Symmetry codes: (i) x, 1/2-y, 1/2+z; (ii) 1-x, -y, -z; (iii) 1-x, 1/2+y, 1/2-z.]
[Figure 3] Fig. 3. Newman projections along the bonds of the O1—C1—C2—C3—C4—O2 chain.
2,2,3,3-tetrafluorobutane-1,4-diol top
Crystal data top
C4H6F4O2F(000) = 328
Mr = 162.09Dx = 1.861 (1) Mg m3
Monoclinic, P21/cMelting point = 355.3–356.3 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 5.4392 (2) ÅCell parameters from 7007 reflections
b = 8.6935 (3) Åθ = 3.1–27.5°
c = 12.4123 (4) ŵ = 0.22 mm1
β = 99.768 (2)°T = 200 K
V = 578.42 (3) Å3Block, colourless
Z = 40.18 × 0.08 × 0.06 mm
Data collection top
Nonius KappaCCD area-detector
diffractometer
1133 reflections with I > 2σ(I)
Radiation source: rotating anodeRint = 0.020
MONTEL, graded multilayered X-ray opticsθmax = 27.5°, θmin = 3.3°
Detector resolution: 9 pixels mm-1h = 77
φ and ω scansk = 1111
2531 measured reflectionsl = 1616
1313 independent 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)] = 0.031Hydrogen site location: difference Fourier map
wR(F2) = 0.085H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0398P)2 + 0.2156P]
where P = (Fo2 + 2Fc2)/3
1313 reflections(Δ/σ)max < 0.001
97 parametersΔρmax = 0.38 e Å3
0 restraintsΔρmin = 0.25 e Å3
Crystal data top
C4H6F4O2V = 578.42 (3) Å3
Mr = 162.09Z = 4
Monoclinic, P21/cMo Kα radiation
a = 5.4392 (2) ŵ = 0.22 mm1
b = 8.6935 (3) ÅT = 200 K
c = 12.4123 (4) Å0.18 × 0.08 × 0.06 mm
β = 99.768 (2)°
Data collection top
Nonius KappaCCD area-detector
diffractometer
1133 reflections with I > 2σ(I)
2531 measured reflectionsRint = 0.020
1313 independent reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.031H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.085Δρmax = 0.38 e Å3
S = 1.04Δρmin = 0.25 e Å3
1313 reflectionsAbsolute structure: ?
97 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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 > 2σ(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*/Ueq
F10.70269 (17)0.39078 (9)0.15846 (6)0.0318 (2)
F21.07701 (15)0.32375 (11)0.13418 (7)0.0343 (2)
F30.81808 (17)0.38903 (11)0.05076 (6)0.0349 (2)
F40.86586 (15)0.14104 (11)0.03922 (6)0.0328 (2)
O10.58505 (19)0.07917 (11)0.18952 (8)0.0256 (2)
H10.528 (4)0.125 (2)0.2357 (16)0.038*
O20.41094 (18)0.23464 (12)0.15572 (7)0.0253 (2)
H20.431 (3)0.143 (2)0.1751 (15)0.038*
C10.8308 (3)0.13254 (16)0.19011 (10)0.0246 (3)
H1A0.92930.05050.16210.030*
H1B0.90990.15560.26620.030*
C20.8355 (2)0.27521 (15)0.12090 (10)0.0216 (3)
C30.7415 (2)0.26145 (14)0.00258 (10)0.0202 (3)
C40.4637 (2)0.24221 (16)0.04003 (10)0.0227 (3)
H4A0.40610.14680.00860.027*
H4B0.37370.33020.01420.027*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0491 (5)0.0227 (4)0.0240 (4)0.0031 (4)0.0075 (4)0.0057 (3)
F20.0285 (4)0.0452 (5)0.0273 (4)0.0150 (4)0.0012 (3)0.0044 (4)
F30.0445 (5)0.0363 (5)0.0227 (4)0.0187 (4)0.0026 (3)0.0077 (3)
F40.0305 (5)0.0407 (5)0.0275 (4)0.0102 (4)0.0059 (3)0.0101 (4)
O10.0327 (5)0.0239 (5)0.0217 (5)0.0053 (4)0.0091 (4)0.0022 (4)
O20.0325 (5)0.0252 (5)0.0169 (4)0.0018 (4)0.0000 (4)0.0003 (4)
C10.0278 (7)0.0261 (7)0.0203 (6)0.0001 (5)0.0051 (5)0.0028 (5)
C20.0226 (6)0.0231 (6)0.0189 (6)0.0036 (5)0.0035 (5)0.0021 (5)
C30.0252 (6)0.0193 (6)0.0171 (6)0.0024 (5)0.0068 (5)0.0004 (5)
C40.0238 (6)0.0274 (7)0.0165 (6)0.0005 (5)0.0024 (5)0.0001 (5)
Geometric parameters (Å, °) top
F1—C21.3651 (15)C1—C21.5114 (18)
F2—C21.3626 (15)C1—H1A0.9900
F3—C31.3587 (14)C1—H1B0.9900
F4—C31.3656 (14)C2—C31.5360 (17)
O1—C11.4135 (17)C3—C41.5128 (17)
O1—H10.80 (2)C4—H4A0.9900
O2—C41.4173 (15)C4—H4B0.9900
O2—H20.84 (2)
C1—O1—H1108.0 (14)C1—C2—C3117.92 (11)
C4—O2—H2108.6 (13)F3—C3—F4105.84 (9)
O1—C1—C2111.96 (11)F3—C3—C4108.66 (10)
O1—C1—H1A109.2F4—C3—C4109.78 (10)
C2—C1—H1A109.2F3—C3—C2107.49 (10)
O1—C1—H1B109.2F4—C3—C2106.97 (10)
C2—C1—H1B109.2C4—C3—C2117.48 (10)
H1A—C1—H1B107.9O2—C4—C3109.65 (10)
F2—C2—F1106.61 (10)O2—C4—H4A109.7
F2—C2—C1107.13 (10)C3—C4—H4A109.7
F1—C2—C1110.41 (10)O2—C4—H4B109.7
F2—C2—C3107.21 (9)C3—C4—H4B109.7
F1—C2—C3106.98 (10)H4A—C4—H4B108.2
O1—C1—C2—F2175.17 (10)C1—C2—C3—F452.09 (14)
O1—C1—C2—F159.45 (14)F2—C2—C3—C4167.32 (11)
O1—C1—C2—C363.91 (14)F1—C2—C3—C453.27 (14)
F2—C2—C3—F344.50 (13)C1—C2—C3—C471.80 (15)
F1—C2—C3—F369.55 (12)F3—C3—C4—O256.60 (13)
C1—C2—C3—F3165.38 (11)F4—C3—C4—O258.71 (13)
F2—C2—C3—F468.79 (12)C2—C3—C4—O2178.82 (11)
F1—C2—C3—F4177.16 (9)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O2i0.80 (2)2.001 (19)2.7972 (14)171.9 (18)
O2—H2···O1ii0.845 (17)1.940 (17)2.7608 (14)163.6 (17)
C1—H1B···F3i0.992.443.2343 (15)137
Symmetry codes: (i) x, −y+1/2, z+1/2; (ii) −x+1, −y, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1···O2i0.80 (2)2.001 (19)2.7972 (14)171.9 (18)
O2—H2···O1ii0.845 (17)1.940 (17)2.7608 (14)163.6 (17)
C1—H1B···F3i0.992.443.2343 (15)137
Symmetry codes: (i) x, −y+1/2, z+1/2; (ii) −x+1, −y, −z.
Acknowledgements top

The authors thank Dr Peter Mayer for technical support. MMR thanks the Fonds der Chemischen Industrie (FCI) for a PhD fellowship.

references
References top

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