Literature DB >> 21837056

1-Bromo-2,3,5,6-tetra-fluoro-4-nitro-benzene.

Mario Stein, Anke Schwarzer, Jürg Hulliger, Edwin Weber.   

Abstract

In the title compound, C(6)BrF(4)NO(2), the nitro group is twisted by 41.7 (3)° with reference to the arene ring mean plane. The main inter-actions stabilizing the crystal structure include O⋯Br contacts [3.150 (2) and 3.201 (2) Å], while F⋯F inter-actions are minor [2.863 (3)-2.908 (3) Å].

Entities:  

Year:  2011        PMID: 21837056      PMCID: PMC3151949          DOI: 10.1107/S160053681102201X

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


Related literature

For halogen inter­actions in mol­ecular crystal structures, see: Awwadi et al. (2006 ▶); Brammer et al. (2001 ▶); Metrangolo et al. (2008 ▶). For fluorine-involved inter­actions, see: Schwarzer et al. (2010 ▶); Merz & Vasylyeva (2010 ▶); Schwarzer & Weber (2008 ▶); Reichenbächer et al. (2005 ▶). For the synthesis, see: Shtark & Shteingarts (1976 ▶).

Experimental

Crystal data

C6BrF4NO2 M = 273.98 Orthorhombic, a = 5.6718 (3) Å b = 10.9476 (6) Å c = 12.2652 (8) Å V = 761.58 (8) Å3 Z = 4 Mo Kα radiation μ = 5.44 mm−1 T = 93 K 0.13 × 0.13 × 0.10 mm

Data collection

Bruker SMART CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2007 ▶) T min = 0.536, T max = 0.612 4314 measured reflections 1550 independent reflections 1447 reflections with I > 2σ(I) R int = 0.026

Refinement

R[F 2 > 2σ(F 2)] = 0.023 wR(F 2) = 0.053 S = 1.00 1550 reflections 127 parameters 1 restraint Δρmax = 0.32 e Å−3 Δρmin = −0.53 e Å−3 Absolute structure: Flack (1983) ▶, 636 Friedel pairs Flack parameter: 0.026 (10) Data collection: SMART (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S160053681102201X/su2278sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102201X/su2278Isup2.hkl Supplementary material file. DOI: 10.1107/S160053681102201X/su2278Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C6BrF4NO2F(000) = 520
Mr = 273.98Dx = 2.390 Mg m3
Orthorhombic, Pna21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2nCell parameters from 2319 reflections
a = 5.6718 (3) Åθ = 3.7–32.8°
b = 10.9476 (6) ŵ = 5.44 mm1
c = 12.2652 (8) ÅT = 93 K
V = 761.58 (8) Å3Needle, colourless
Z = 40.13 × 0.13 × 0.10 mm
Bruker SMART CCD area-detector diffractometer1550 independent reflections
Radiation source: fine-focus sealed tube1447 reflections with I > 2σ(I)
graphiteRint = 0.026
phi and ω scansθmax = 27.5°, θmin = 2.5°
Absorption correction: multi-scan (SADABS; Bruker, 2007)h = −7→7
Tmin = 0.536, Tmax = 0.612k = −14→12
4314 measured reflectionsl = −15→15
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.023w = 1/[σ2(Fo2) + (0.0208P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.053(Δ/σ)max = 0.008
S = 1.00Δρmax = 0.32 e Å3
1550 reflectionsΔρmin = −0.53 e Å3
127 parametersAbsolute structure: Flack (1983), 636 Friedel pairs
1 restraintFlack parameter: 0.026 (10)
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.
xyzUiso*/Ueq
Br11.16169 (4)0.62891 (2)0.12241 (5)0.01760 (10)
F10.9560 (3)0.69267 (15)−0.10033 (17)0.0188 (4)
F20.6066 (3)0.58458 (16)−0.20909 (18)0.0178 (4)
F30.5004 (3)0.30738 (15)0.08418 (15)0.0181 (4)
F40.8565 (3)0.41466 (18)0.19058 (19)0.0192 (4)
N10.3610 (4)0.3813 (2)−0.1276 (3)0.0148 (6)
O10.3925 (4)0.36408 (18)−0.2245 (2)0.0181 (5)
O20.1833 (3)0.3518 (2)−0.0760 (2)0.0207 (6)
C10.8465 (4)0.5971 (3)−0.0542 (3)0.0134 (7)
C20.6671 (4)0.5405 (3)−0.1118 (3)0.0136 (7)
C30.5498 (4)0.4424 (3)−0.0658 (3)0.0128 (7)
C40.6105 (5)0.4023 (3)0.0374 (3)0.0146 (7)
C50.7936 (4)0.4574 (3)0.0933 (3)0.0129 (8)
C60.9119 (4)0.5558 (3)0.0468 (3)0.0146 (7)
U11U22U33U12U13U23
Br10.01516 (11)0.01875 (15)0.01890 (19)−0.00140 (8)−0.00323 (18)−0.0046 (2)
F10.0214 (7)0.0153 (9)0.0198 (13)−0.0066 (6)0.0011 (8)0.0038 (8)
F20.0241 (8)0.0159 (9)0.0135 (13)−0.0005 (7)−0.0031 (9)0.0027 (9)
F30.0224 (7)0.0155 (9)0.0164 (12)−0.0057 (6)0.0040 (8)0.0017 (7)
F40.0256 (9)0.0177 (10)0.0142 (14)0.0018 (7)−0.0024 (8)0.0009 (9)
N10.0150 (12)0.0158 (15)0.014 (2)−0.0005 (8)−0.0002 (11)−0.0015 (13)
O10.0205 (8)0.0206 (12)0.0133 (16)−0.0014 (7)−0.0005 (10)−0.0048 (10)
O20.0134 (9)0.0245 (14)0.0241 (17)−0.0025 (7)0.0025 (10)−0.0016 (11)
C10.0165 (12)0.0082 (15)0.016 (2)−0.0009 (10)0.0038 (13)0.0006 (13)
C20.0160 (12)0.0125 (16)0.012 (2)0.0048 (9)0.0001 (12)−0.0004 (14)
C30.0099 (10)0.0143 (15)0.014 (2)0.0018 (10)0.0001 (12)−0.0040 (13)
C40.0169 (12)0.0107 (15)0.016 (2)0.0019 (10)0.0045 (13)0.0003 (13)
C50.0150 (10)0.0158 (15)0.008 (2)0.0030 (9)0.0001 (11)−0.0003 (12)
C60.0110 (10)0.0169 (15)0.016 (2)0.0014 (10)−0.0020 (12)−0.0065 (13)
Br1—C61.874 (3)F4—F3iii2.877 (2)
Br1—O1i3.150 (2)F4—F2vii2.901 (2)
Br1—O1ii3.201 (2)N1—O11.217 (4)
F3—O2iii2.823 (3)N1—O21.234 (3)
F1—C11.342 (3)N1—C31.472 (4)
F1—F2iv2.908 (3)O1—Br1ix3.150 (2)
F2—C21.332 (4)O1—Br1x3.201 (2)
F2—F3v2.863 (3)O2—F3viii2.823 (3)
F2—F4v2.901 (2)C1—C61.369 (5)
F2—F1vi2.908 (3)C1—C21.385 (4)
F3—C41.341 (3)C2—C31.385 (4)
F3—F2vii2.863 (3)C3—C41.383 (5)
F3—F4viii2.877 (2)C4—C51.382 (4)
F4—C51.331 (4)C5—C61.391 (4)
C6—Br1—O1i155.87 (10)N1—O1—Br1ix134.13 (18)
C6—Br1—O1ii124.16 (9)N1—O1—Br1x133.10 (18)
O1i—Br1—O1ii73.03 (6)Br1ix—O1—Br1x75.36 (6)
C1—F1—F2iv169.53 (15)N1—O2—F3viii144.98 (19)
C2—F2—F3v176.03 (17)F1—C1—C6120.9 (3)
C2—F2—F4v127.90 (16)F1—C1—C2118.2 (3)
F3v—F2—F4v55.33 (6)C6—C1—C2120.8 (3)
C2—F2—F1vi88.19 (17)F2—C2—C3121.5 (3)
F3v—F2—F1vi89.86 (7)F2—C2—C1119.0 (3)
F4v—F2—F1vi85.76 (7)C3—C2—C1119.5 (3)
C4—F3—O2iii90.56 (18)C4—C3—C2120.0 (3)
C4—F3—F2vii99.04 (18)C4—C3—N1120.6 (3)
O2iii—F3—F2vii161.63 (9)C2—C3—N1119.5 (3)
C4—F3—F4viii168.70 (16)F3—C4—C5118.4 (3)
O2iii—F3—F4viii84.17 (8)F3—C4—C3121.4 (3)
F2vii—F3—F4viii83.52 (8)C5—C4—C3120.1 (3)
C5—F4—F3iii88.06 (17)F4—C5—C4119.5 (3)
C5—F4—F2vii97.86 (13)F4—C5—C6120.7 (3)
F3iii—F4—F2vii116.85 (8)C4—C5—C6119.8 (3)
O1—N1—O2125.5 (3)C1—C6—C5119.7 (3)
O1—N1—C3117.8 (2)C1—C6—Br1120.8 (2)
O2—N1—C3116.6 (3)C5—C6—Br1119.5 (2)
O2—N1—O1—Br1ix−164.81 (19)F4viii—F3—C4—C5−50.3 (12)
C3—N1—O1—Br1ix15.2 (4)O2iii—F3—C4—C365.5 (3)
O2—N1—O1—Br1x−49.6 (4)F2vii—F3—C4—C3−130.3 (3)
C3—N1—O1—Br1x130.4 (2)F4viii—F3—C4—C3127.4 (9)
O1—N1—O2—F3viii110.3 (4)C2—C3—C4—F3−179.9 (3)
C3—N1—O2—F3viii−69.7 (4)N1—C3—C4—F30.0 (4)
F2iv—F1—C1—C6−133.4 (10)C2—C3—C4—C5−2.2 (4)
F2iv—F1—C1—C247.2 (13)N1—C3—C4—C5177.7 (3)
F3v—F2—C2—C3174 (2)F3iii—F4—C5—C465.3 (3)
F4v—F2—C2—C330.2 (4)F2vii—F4—C5—C4−51.5 (3)
F1vi—F2—C2—C3113.4 (3)F3iii—F4—C5—C6−113.9 (3)
F3v—F2—C2—C1−4(3)F2vii—F4—C5—C6129.2 (2)
F4v—F2—C2—C1−147.6 (2)F3—C4—C5—F40.5 (4)
F1vi—F2—C2—C1−64.4 (3)C3—C4—C5—F4−177.2 (2)
F1—C1—C2—F2−1.5 (4)F3—C4—C5—C6179.8 (3)
C6—C1—C2—F2179.1 (3)C3—C4—C5—C62.0 (4)
F1—C1—C2—C3−179.4 (3)F1—C1—C6—C5179.2 (3)
C6—C1—C2—C31.2 (4)C2—C1—C6—C5−1.4 (4)
F2—C2—C3—C4−177.2 (3)F1—C1—C6—Br1−1.6 (4)
C1—C2—C3—C40.6 (4)C2—C1—C6—Br1177.8 (2)
F2—C2—C3—N12.9 (4)F4—C5—C6—C1179.0 (3)
C1—C2—C3—N1−179.2 (3)C4—C5—C6—C1−0.2 (4)
O1—N1—C3—C4−138.6 (3)F4—C5—C6—Br1−0.2 (4)
O2—N1—C3—C441.4 (4)C4—C5—C6—Br1−179.4 (2)
O1—N1—C3—C241.3 (4)O1i—Br1—C6—C1−143.2 (2)
O2—N1—C3—C2−138.7 (3)O1ii—Br1—C6—C186.1 (3)
O2iii—F3—C4—C5−112.3 (3)O1i—Br1—C6—C536.0 (4)
F2vii—F3—C4—C552.0 (3)O1ii—Br1—C6—C5−94.7 (2)
  3 in total

1.  The nature of halogen...halogen synthons: crystallographic and theoretical studies.

Authors:  Firas F Awwadi; Roger D Willett; Kirk A Peterson; Brendan Twamley
Journal:  Chemistry       Date:  2006-12-04       Impact factor: 5.236

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

Review 3.  Fluorine in crystal engineering--"the little atom that could".

Authors:  Katharina Reichenbächer; Heike I Süss; Jurg Hulliger
Journal:  Chem Soc Rev       Date:  2004-12-01       Impact factor: 54.564

  3 in total
  1 in total

1.  Anomalous halogen bonds in the crystal structures of 1,2,3-tri-bromo-5-nitro-benzene and 1,3-di-bromo-2-iodo-5-nitro-benzene.

Authors:  José A Romero; Gerardo Aguirre Hernández; Sylvain Bernès
Journal:  Acta Crystallogr E Crystallogr Commun       Date:  2015-07-22
  1 in total

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