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The title compound, C12H7Br3O, belongs to a group of flame retardants known as polybrominated di­phenyl ethers (PBDE). Salient features of the packing of the title compound are infinite intermolecular Br...Br contact chains along the b direction.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802008693/bt6146sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802008693/bt6146Isup2.hkl
Contains datablock I

CCDC reference: 189413

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.006 Å
  • R factor = 0.035
  • wR factor = 0.044
  • Data-to-parameter ratio = 17.3

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
RINTA_01 Alert C The value of Rint is greater than 0.10 Rint given 0.103
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Computing details top

Data collection: EXPOSE in IPDS (Stoe, 1997); cell refinement: CELL in IPDS; data reduction: INTEGRATE in IPDS and X-RED (Stoe, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Bergerhoff, 1996).

2,4-Bibromophenyl 4-bromophenyl ether top
Crystal data top
C12H7Br3ODx = 2.092 Mg m3
Mr = 406.91Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1235 reflections
a = 15.480 (3) Åθ = 1.7–26.0°
b = 5.9692 (9) ŵ = 9.34 mm1
c = 27.962 (5) ÅT = 293 K
V = 2583.7 (8) Å3Irregular, colourless
Z = 80.16 × 0.07 × 0.06 mm
F(000) = 1536
Data collection top
Stoe IPDS area-detector
diffractometer
2513 independent reflections
Radiation source: fine-focus sealed tube1335 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.103
Detector resolution: 6.0 pixels mm-1θmax = 26.0°, θmin = 2.0°
area detector scansh = 1919
Absorption correction: numerical
(XRED; Stoe & Cie, 1997)
k = 77
Tmin = 0.231, Tmax = 0.574l = 3434
36351 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)] = 0.035Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.044H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.01P)2]
where P = (Fo2 + 2Fc2)/3
2513 reflections(Δ/σ)max < 0.001
145 parametersΔρmax = 0.53 e Å3
40 restraintsΔρmin = 0.41 e Å3
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*/Ueq
Br10.64870 (3)0.19445 (13)0.165844 (15)0.0833 (2)
Br20.67846 (2)0.17074 (10)0.415110 (16)0.06006 (14)
Br30.34387 (3)0.32515 (11)0.486260 (15)0.06214 (16)
O0.59364 (19)0.2643 (5)0.37919 (10)0.0590 (9)
C10.6023 (2)0.2375 (8)0.33024 (14)0.0447 (12)
C20.5668 (3)0.0669 (8)0.30430 (16)0.0560 (13)
H20.53300.04020.31960.067*
C30.5806 (3)0.0519 (8)0.25538 (16)0.0556 (13)
H30.55680.06570.23800.067*
C40.6295 (2)0.2111 (9)0.23291 (14)0.0508 (12)
C50.6660 (3)0.3846 (8)0.25861 (15)0.0587 (13)
H50.69940.49230.24330.070*
C60.6522 (3)0.3965 (8)0.30768 (15)0.0542 (13)
H60.67680.51220.32530.065*
C70.5366 (3)0.1259 (8)0.40292 (13)0.0467 (12)
C80.5628 (2)0.0757 (8)0.42236 (13)0.0408 (11)
C90.5069 (2)0.2116 (8)0.44708 (12)0.0384 (11)
H90.52510.34830.45940.046*
C100.4222 (2)0.1388 (8)0.45310 (13)0.0411 (12)
C110.3956 (3)0.0634 (9)0.43452 (15)0.0537 (13)
H110.33880.11030.43870.064*
C120.4526 (3)0.1959 (9)0.40987 (15)0.0557 (11)
H120.43470.33340.39780.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.0966 (4)0.1040 (6)0.0492 (3)0.0095 (5)0.0052 (3)0.0010 (3)
Br20.0372 (2)0.0669 (3)0.0761 (3)0.0025 (3)0.0028 (2)0.0101 (3)
Br30.0481 (2)0.0738 (4)0.0645 (3)0.0102 (3)0.0116 (2)0.0004 (3)
O0.080 (2)0.049 (3)0.0477 (16)0.0253 (17)0.0002 (14)0.0012 (16)
C10.047 (2)0.045 (4)0.043 (2)0.007 (3)0.003 (2)0.004 (2)
C20.059 (3)0.052 (4)0.057 (3)0.022 (3)0.004 (2)0.002 (3)
C30.058 (3)0.054 (3)0.054 (3)0.014 (3)0.008 (2)0.011 (3)
C40.041 (2)0.052 (4)0.059 (2)0.001 (2)0.004 (2)0.009 (3)
C50.052 (3)0.057 (4)0.068 (3)0.016 (3)0.004 (2)0.009 (2)
C60.064 (3)0.040 (4)0.058 (3)0.018 (3)0.010 (3)0.007 (2)
C70.061 (3)0.041 (4)0.038 (2)0.011 (2)0.001 (2)0.004 (2)
C80.039 (2)0.044 (3)0.040 (3)0.011 (2)0.0034 (19)0.002 (2)
C90.040 (2)0.032 (3)0.043 (2)0.003 (2)0.0067 (17)0.003 (2)
C100.038 (2)0.048 (4)0.038 (2)0.001 (2)0.0022 (17)0.005 (2)
C110.043 (3)0.059 (4)0.059 (3)0.011 (3)0.000 (2)0.003 (3)
C120.064 (3)0.044 (3)0.058 (2)0.015 (3)0.007 (3)0.009 (3)
Geometric parameters (Å, º) top
Br1—C41.901 (4)C7—C81.381 (5)
Br2—C81.889 (4)C8—C91.373 (5)
Br3—C101.889 (4)C9—C101.391 (5)
O—C71.380 (5)C10—C111.377 (6)
O—C11.385 (4)C11—C121.371 (6)
C1—C21.365 (6)C2—H20.9300
C1—C61.377 (6)C3—H30.9300
C2—C31.387 (6)C5—H50.9300
C3—C41.368 (6)C6—H60.9300
C4—C51.381 (6)C9—H90.9300
C5—C61.391 (5)C11—H110.9300
C7—C121.378 (5)C12—H120.9300
C7—O—C1117.9 (3)C11—C10—Br3120.6 (3)
C2—C1—C6119.8 (4)C9—C10—Br3118.7 (4)
C2—C1—O124.9 (4)C12—C11—C10120.2 (4)
C6—C1—O115.3 (4)C11—C12—C7120.2 (5)
C1—C2—C3120.6 (4)C1—C2—H2119.7
C4—C3—C2119.6 (4)C3—C2—H2119.7
C3—C4—C5120.6 (4)C4—C3—H3120.2
C3—C4—Br1120.2 (4)C2—C3—H3120.2
C5—C4—Br1119.2 (3)C4—C5—H5120.4
C4—C5—C6119.3 (4)C6—C5—H5120.4
C1—C6—C5120.2 (4)C1—C6—H6119.9
C12—C7—O119.3 (4)C5—C6—H6119.9
C12—C7—C8119.0 (4)C8—C9—H9121.0
O—C7—C8121.5 (4)C10—C9—H9121.0
C9—C8—C7121.9 (4)C12—C11—H11119.9
C9—C8—Br2118.3 (3)C10—C11—H11119.9
C7—C8—Br2119.9 (3)C11—C12—H12119.9
C8—C9—C10118.0 (4)C7—C12—H12119.9
C11—C10—C9120.7 (4)
C7—O—C1—C28.5 (6)C12—C7—C8—C92.1 (6)
C7—O—C1—C6172.7 (4)O—C7—C8—C9178.3 (3)
C6—C1—C2—C30.1 (7)C12—C7—C8—Br2177.9 (3)
O—C1—C2—C3178.7 (4)O—C7—C8—Br21.8 (5)
C1—C2—C3—C40.7 (7)C7—C8—C9—C101.3 (6)
C2—C3—C4—C50.8 (6)Br2—C8—C9—C10178.8 (3)
C2—C3—C4—Br1179.6 (3)C8—C9—C10—C110.3 (6)
C3—C4—C5—C60.3 (6)C8—C9—C10—Br3179.1 (3)
Br1—C4—C5—C6179.8 (3)C9—C10—C11—C120.1 (6)
C2—C1—C6—C50.5 (7)Br3—C10—C11—C12179.0 (3)
O—C1—C6—C5179.3 (4)C10—C11—C12—C71.0 (7)
C4—C5—C6—C10.4 (6)O—C7—C12—C11178.2 (4)
C1—O—C7—C1292.7 (5)C8—C7—C12—C112.0 (6)
C1—O—C7—C891.2 (5)
 

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