Literature DB >> 21578279

1,2,3-Trifluoro-benzene.

Michael T Kirchner, Dieter Bläser, Roland Boese, Tejender S Thakur, Gautam R Desiraju.   

Abstract

In the title compound, C(6)H(3)F(3), weak electrostatic and dispersive forces between C(δ+)-F(δ-) and H(δ+)-C(δ-) groups are at the borderline of the hydrogen-bond phenomenon and are poorly directional and further deformed in the presence of π-π stacking inter-actions. The mol-ecule lies on a twofold rotation axis. In the crystal structure, one-dimensional tapes are formed via two anti-dromic C-H⋯F hydrogen bonds. These tapes are, in turn, connected into corrugated two-dimensional sheets by bifurcated C-H⋯F hydrogen bonds. Packing in the third dimension is furnished by π-π stacking inter-actions with a centroid-centroid distance of 3.6362 (14) Å.

Entities:  

Year:  2009        PMID: 21578279      PMCID: PMC2971369          DOI: 10.1107/S1600536809038975

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For C—H⋯F inter­actions, see: Althoff et al. (2006 ▶); Bats et al. (2000 ▶); Choudhury et al. (2004 ▶); D’Oria & Novoa (2008 ▶); Dunitz & Taylor (1997 ▶); Howard et al. (1996 ▶); Müller et al. (2007 ▶); O’Hagan (2008 ▶); Reichenbacher et al. (2005 ▶); Weiss et al. (1997 ▶). For related crystal structures of several polyfluorinated benzenes, see: Thalladi et al. (1998 ▶). For crystallization techniques, see: Boese & Nussbaumer (1994 ▶).

Experimental

Crystal data

C6H3F3 M = 132.08 Monoclinic, a = 7.4238 (19) Å b = 11.590 (3) Å c = 7.0473 (17) Å β = 112.783 (4)° V = 559.1 (2) Å3 Z = 4 Mo Kα radiation μ = 0.16 mm−1 T = 233 K 0.30 × 0.30 × 0.30 mm

Data collection

Siemens SMART three-axis goniometer with an APEXII area-detector system diffractometer Absorption correction: multi-scan (SADABS; Bruker; 2004 ▶) T min = 0.820, T max = 0.953 1074 measured reflections 634 independent reflections 413 reflections with I > 2σ(I) R int = 0.013

Refinement

R[F 2 > 2σ(F 2)] = 0.061 wR(F 2) = 0.226 S = 1.04 634 reflections 44 parameters H-atom parameters constrained Δρmax = 0.20 e Å−3 Δρmin = −0.18 e Å−3 Data collection: APEX2 (Bruker, 2008 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: Mercury (Macrae et al., 2008 ▶) and GIMP2 (The GIMP team, 2008 ▶); software used to prepare material for publication: publCIF (Westrip, 2009 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809038975/lh2880sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809038975/lh2880Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C6H3F3F(000) = 264
Mr = 132.08Dx = 1.569 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 376 reflections
a = 7.4238 (19) Åθ = 3.8–22.7°
b = 11.590 (3) ŵ = 0.16 mm1
c = 7.0473 (17) ÅT = 233 K
β = 112.783 (4)°Cylindric, colourless
V = 559.1 (2) Å30.30 × 0.30 × 0.30 mm
Z = 4
Siemens SMART three-axis goniometer with an APEXII area-detector system diffractometer634 independent reflections
Radiation source: fine-focus sealed tube413 reflections with I > 2σ(I)
graphiteRint = 0.013
Detector resolution: 512 pixels mm-1θmax = 28.2°, θmin = 3.5°
in ω at 0.3° scan width one run with 740 frames, phi = 0°, chi = 0°h = −9→9
Absorption correction: multi-scan (SADABS; Bruker; 2004)k = −14→10
Tmin = 0.820, Tmax = 0.953l = −9→4
1074 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.061Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.226H-atom parameters constrained
S = 1.04w = 1/[σ2(Fo2) + (0.1501P)2 + 0.039P], where P = (Fo2 + 2Fc2)/3
634 reflections(Δ/σ)max = 0.017
44 parametersΔρmax = 0.20 e Å3
0 restraintsΔρmin = −0.18 e Å3
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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
F11.00000.30558 (17)0.25000.1156 (10)
F20.6666 (2)0.4183 (2)0.1576 (3)0.1354 (10)
C11.00000.4213 (3)0.25000.0769 (9)
C20.8308 (3)0.4803 (2)0.2036 (3)0.0824 (8)
C30.8265 (4)0.5973 (3)0.2023 (3)0.0942 (9)
H30.68330.63880.15850.113*
C41.00000.6558 (3)0.25000.1006 (13)
H41.00000.74220.25000.121*
U11U22U33U12U13U23
F10.161 (2)0.0623 (13)0.1249 (16)0.0000.0563 (14)0.000
F20.0959 (12)0.157 (2)0.1484 (16)−0.0341 (10)0.0415 (10)0.0067 (12)
C10.1030 (19)0.0573 (16)0.0725 (15)0.0000.0364 (13)0.000
C20.0830 (14)0.0890 (17)0.0770 (13)−0.0101 (9)0.0327 (10)0.0013 (9)
C30.1073 (17)0.0935 (18)0.0858 (15)0.0277 (12)0.0419 (12)0.0094 (10)
C40.163 (4)0.0605 (17)0.0848 (19)0.0000.056 (2)0.000
F1—C11.341 (4)C3—C41.377 (3)
F2—C21.342 (3)C3—H31.0973
C1—C21.354 (3)C4—H41.0018
C2—C31.357 (4)
F1—C1—C2120.30 (15)C2—C3—H3117.3
C2i—C1—C2119.4 (3)C4—C3—H3124.4
F2—C2—C3121.1 (2)C3—C4—C3i121.0 (3)
F2—C2—C1117.3 (3)C3—C4—H4119.5
C3—C2—C1121.5 (2)C3i—C4—H4119.5
C2—C3—C4118.3 (2)
D—H···AD—HH···AD···AD—H···A
C3—H3···F2ii1.102.773.560 (3)129
C3—H3···F1iii1.102.593.528 (4)144
C4—H4···F2iv1.002.603.440 (4)142
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C3—H3⋯F2i1.102.773.560 (3)129
C3—H3⋯F1ii1.102.593.528 (4)144
C4—H4⋯F2iii1.002.603.440 (4)142

Symmetry codes: (i) ; (ii) ; (iii) .

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