Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 11;67(Pt 7):o1604. doi: 10.1107/S1600536811020721

4,5,6,7-Tetra­chloro-N-(2,3,4-trifluoro­phen­yl)phthalimide

Yin-Jun Zhang a, Chen-Tao Luo a, Yu-Guang Wang a, Zhao Wang a,*
PMCID: PMC3151790  PMID: 21837012

Abstract

The asymmetric unit of the title compound, C14H2Cl4F3NO2, contains two independent mol­ecules. In each mol­ecule, the phthalimide ring system is nearly planar [maximum atomic deviation = 0.031 (2) or 0.038 (2) Å] and oriented with respect to the benzene ring at 65.04 (7) or 71.76 (10)°. Weak inter­molecular C—H⋯O and C—H⋯F hydrogen bonding is present in the crystal structure.

Related literature

For the title compound as an inter­mediate of organic electro-luminescent materials, see: Han & Kay (2005). For the synthesis, see: Valkonen et al. (2007); Barchin et al. (2002). For related structures, see: Xu et al. (2006); Fu et al. (2010a ,b ,c ).graphic file with name e-67-o1604-scheme1.jpg

Experimental

Crystal data

  • C14H2Cl4F3NO2

  • M r = 414.97

  • Triclinic, Inline graphic

  • a = 6.7722 (7) Å

  • b = 8.8052 (12) Å

  • c = 24.493 (3) Å

  • α = 95.777 (9)°

  • β = 94.514 (17)°

  • γ = 98.839 (12)°

  • V = 1429.2 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.87 mm−1

  • T = 113 K

  • 0.20 × 0.18 × 0.12 mm

Data collection

  • Rigaku Saturn 724CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2001) T min = 0.845, T max = 0.903

  • 13490 measured reflections

  • 6684 independent reflections

  • 4832 reflections with I > 2σ(I)

  • R int = 0.033

Refinement

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.095

  • S = 0.98

  • 6684 reflections

  • 433 parameters

  • H-atom parameters constrained

  • Δρmax = 0.62 e Å−3

  • Δρmin = −0.38 e Å−3

Data collection: SMART (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811020721/xu5228sup1.cif

e-67-o1604-sup1.cif (25.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811020721/xu5228Isup2.hkl

e-67-o1604-Isup2.hkl (327.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811020721/xu5228Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C14—H14⋯O3i 0.95 2.44 3.210 (3) 138
C27—H27⋯F3ii 0.95 2.45 3.379 (3) 165
C28—H28⋯O1 0.95 2.50 3.403 (3) 158

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

supplementary crystallographic information

Comment

The title compound is a key intermediate of organic electro-luminescent, the emission of light by organic molecules exposed in the electric field, which has been wide investigated in academic and industrial displays (Han & Kay, 2005).

The molecular structure of the title compound is illustrated in Fig. 1. In the title compound, two rings are nearly planar, but the molecule as a whole is not planar. The dihedral angle between the benzene ring and the phthalimide plane is 66.03 (12) °, which is greater than 60.3 (5)° found in a related compound 2-(2-iodoethyl)isoindole-1,3-dione (Valkonen et al. 2007). Intermolecular weak C—H···O and C—H···F hydrogen bonding is present in the crystal structure (Table 1).

Experimental

Compound (I) was prepared according to the procedure in the literature (Barchin et al., 2002). The reaction was initiated by the addition of one molar equivalent of 2,3,4-trifluoroaniline and one molar equivalents of 4,5,6,7-tetrachlorophthalic anhydride and subsequent refluxing overnight, and then filtered. The crude produce was washed with water three times, and dried. The compound resulted (yield 96%) and single crystals suitable for X-ray analysis were obtained by slow evaporation of a ethyl acetate solution.

Refinement

H atoms were positioned geometrically and refined as riding with C—H = 0.95 Å, and Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

View of the molecule of showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.

Crystal data

C14H2Cl4F3NO2 Z = 4
Mr = 414.97 F(000) = 816
Triclinic, P1 Dx = 1.928 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 6.7722 (7) Å Cell parameters from 4943 reflections
b = 8.8052 (12) Å θ = 1.7–27.9°
c = 24.493 (3) Å µ = 0.87 mm1
α = 95.777 (9)° T = 113 K
β = 94.514 (17)° Prism, colorless
γ = 98.839 (12)° 0.20 × 0.18 × 0.12 mm
V = 1429.2 (3) Å3

Data collection

Rigaku Saturn 724CCD area-detector diffractometer 6684 independent reflections
Radiation source: rotating anode 4832 reflections with I > 2σ(I)
multilayer Rint = 0.033
Detector resolution: 14.22 pixels mm-1 θmax = 27.9°, θmin = 1.7°
ω and φ scans h = −8→8
Absorption correction: multi-scan (SADABS; Bruker, 2001) k = −11→11
Tmin = 0.845, Tmax = 0.903 l = −31→32
13490 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.095 H-atom parameters constrained
S = 0.98 w = 1/[σ2(Fo2) + (0.0384P)2] where P = (Fo2 + 2Fc2)/3
6684 reflections (Δ/σ)max = 0.001
433 parameters Δρmax = 0.62 e Å3
0 restraints Δρmin = −0.38 e Å3

Special details

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)

x y z Uiso*/Ueq
Cl1 0.32227 (8) 0.91214 (6) 0.18882 (2) 0.01916 (13)
Cl2 0.25294 (9) 0.79727 (7) 0.06239 (2) 0.02243 (14)
Cl3 0.24340 (8) 0.44993 (7) 0.02105 (2) 0.02233 (13)
Cl4 0.28079 (8) 0.20952 (6) 0.10536 (2) 0.01886 (13)
Cl5 0.83636 (8) 1.38342 (6) 0.20872 (2) 0.01938 (13)
Cl6 0.77697 (8) 1.27830 (6) 0.08171 (2) 0.02106 (13)
Cl7 0.75697 (8) 0.93290 (7) 0.03745 (2) 0.02244 (14)
Cl8 0.78622 (8) 0.68379 (6) 0.11969 (2) 0.01849 (13)
F1 0.09797 (18) 0.52932 (15) 0.35163 (5) 0.0272 (3)
F2 0.1377 (2) 0.44755 (17) 0.45515 (5) 0.0370 (4)
F3 0.4616 (2) 0.32808 (17) 0.48974 (5) 0.0351 (4)
F4 1.29401 (19) 1.04373 (16) 0.33909 (5) 0.0290 (3)
F5 1.4227 (2) 0.98029 (18) 0.44020 (6) 0.0427 (4)
F6 1.1612 (2) 0.82690 (18) 0.50178 (5) 0.0442 (4)
O1 0.3982 (2) 0.74947 (18) 0.29461 (6) 0.0233 (4)
O2 0.3402 (2) 0.23349 (17) 0.23416 (6) 0.0229 (4)
O3 0.9291 (2) 1.21384 (18) 0.31271 (6) 0.0216 (4)
O4 0.8648 (2) 0.70099 (18) 0.24803 (6) 0.0257 (4)
N1 0.3776 (3) 0.4840 (2) 0.27781 (7) 0.0171 (4)
N2 0.9077 (3) 0.9487 (2) 0.29353 (7) 0.0177 (4)
C1 0.3739 (3) 0.6333 (3) 0.26336 (9) 0.0176 (5)
C2 0.3363 (3) 0.6123 (2) 0.20166 (8) 0.0151 (5)
C3 0.3126 (3) 0.7200 (2) 0.16569 (9) 0.0163 (5)
C4 0.2817 (3) 0.6680 (3) 0.10912 (8) 0.0168 (5)
C5 0.2751 (3) 0.5115 (3) 0.09030 (8) 0.0166 (5)
C6 0.2956 (3) 0.4031 (2) 0.12762 (8) 0.0164 (5)
C7 0.3259 (3) 0.4568 (3) 0.18312 (8) 0.0160 (5)
C8 0.3474 (3) 0.3692 (3) 0.23222 (8) 0.0169 (5)
C9 0.4061 (3) 0.4492 (2) 0.33327 (8) 0.0180 (5)
C10 0.2611 (3) 0.4700 (3) 0.36825 (9) 0.0208 (5)
C11 0.2802 (3) 0.4284 (3) 0.42102 (9) 0.0241 (5)
C12 0.4469 (4) 0.3681 (3) 0.43799 (9) 0.0254 (6)
C13 0.5958 (4) 0.3496 (3) 0.40436 (9) 0.0251 (6)
H13 0.7109 0.3090 0.4171 0.030*
C14 0.5749 (3) 0.3914 (3) 0.35132 (9) 0.0211 (5)
H14 0.6769 0.3802 0.3274 0.025*
C15 0.8977 (3) 1.0995 (3) 0.28042 (8) 0.0165 (5)
C16 0.8468 (3) 1.0809 (2) 0.21917 (8) 0.0155 (5)
C17 0.8229 (3) 1.1919 (2) 0.18423 (8) 0.0167 (5)
C18 0.7927 (3) 1.1435 (3) 0.12721 (8) 0.0171 (5)
C19 0.7833 (3) 0.9880 (3) 0.10714 (8) 0.0170 (5)
C20 0.8001 (3) 0.8765 (2) 0.14369 (8) 0.0155 (5)
C21 0.8327 (3) 0.9259 (2) 0.19943 (8) 0.0155 (5)
C22 0.8675 (3) 0.8368 (3) 0.24746 (8) 0.0169 (5)
C23 0.9670 (3) 0.9153 (2) 0.34779 (8) 0.0189 (5)
C24 1.1641 (3) 0.9649 (3) 0.36851 (9) 0.0209 (5)
C25 1.2298 (4) 0.9340 (3) 0.42078 (9) 0.0257 (6)
C26 1.0962 (4) 0.8546 (3) 0.45089 (9) 0.0294 (6)
C27 0.8992 (4) 0.8043 (3) 0.43104 (9) 0.0316 (6)
H27 0.8088 0.7490 0.4526 0.038*
C28 0.8346 (4) 0.8359 (3) 0.37858 (9) 0.0254 (5)
H28 0.6988 0.8026 0.3641 0.031*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0216 (3) 0.0129 (3) 0.0235 (3) 0.0040 (2) 0.0019 (2) 0.0027 (2)
Cl2 0.0282 (3) 0.0206 (3) 0.0198 (3) 0.0039 (3) 0.0020 (2) 0.0088 (2)
Cl3 0.0299 (3) 0.0228 (3) 0.0139 (2) 0.0036 (3) 0.0013 (2) 0.0017 (2)
Cl4 0.0233 (3) 0.0144 (3) 0.0185 (3) 0.0032 (2) 0.0022 (2) −0.0004 (2)
Cl5 0.0240 (3) 0.0126 (3) 0.0220 (3) 0.0042 (2) 0.0030 (2) 0.0020 (2)
Cl6 0.0251 (3) 0.0195 (3) 0.0201 (3) 0.0044 (2) 0.0025 (2) 0.0083 (2)
Cl7 0.0308 (3) 0.0228 (3) 0.0136 (3) 0.0044 (3) 0.0018 (2) 0.0017 (2)
Cl8 0.0228 (3) 0.0142 (3) 0.0179 (3) 0.0029 (2) 0.0021 (2) −0.0008 (2)
F1 0.0239 (7) 0.0282 (8) 0.0303 (7) 0.0102 (6) 0.0008 (6) 0.0002 (6)
F2 0.0414 (9) 0.0446 (10) 0.0289 (8) 0.0109 (8) 0.0184 (7) 0.0044 (7)
F3 0.0549 (10) 0.0372 (10) 0.0147 (7) 0.0081 (8) 0.0041 (7) 0.0084 (6)
F4 0.0300 (8) 0.0265 (8) 0.0295 (8) −0.0009 (6) 0.0030 (6) 0.0068 (6)
F5 0.0369 (9) 0.0459 (11) 0.0404 (9) −0.0005 (8) −0.0177 (7) 0.0088 (8)
F6 0.0619 (11) 0.0490 (11) 0.0223 (8) 0.0097 (9) −0.0087 (7) 0.0154 (7)
O1 0.0322 (10) 0.0181 (9) 0.0186 (8) 0.0070 (8) −0.0033 (7) −0.0026 (7)
O2 0.0354 (10) 0.0141 (9) 0.0192 (8) 0.0041 (7) 0.0022 (7) 0.0026 (6)
O3 0.0298 (9) 0.0161 (9) 0.0179 (8) 0.0053 (7) 0.0002 (7) −0.0031 (6)
O4 0.0417 (11) 0.0150 (9) 0.0202 (8) 0.0056 (8) 0.0000 (8) 0.0019 (7)
N1 0.0248 (10) 0.0137 (10) 0.0130 (9) 0.0047 (8) 0.0000 (8) 0.0013 (7)
N2 0.0267 (11) 0.0128 (10) 0.0137 (9) 0.0038 (8) 0.0002 (8) 0.0019 (7)
C1 0.0191 (12) 0.0163 (12) 0.0173 (11) 0.0046 (10) −0.0019 (9) 0.0014 (9)
C2 0.0131 (11) 0.0154 (12) 0.0162 (10) 0.0013 (9) 0.0005 (9) 0.0019 (8)
C3 0.0146 (11) 0.0124 (11) 0.0215 (11) 0.0018 (9) 0.0020 (9) 0.0009 (9)
C4 0.0155 (11) 0.0168 (12) 0.0183 (11) 0.0015 (9) 0.0009 (9) 0.0062 (9)
C5 0.0160 (11) 0.0182 (12) 0.0153 (10) 0.0006 (9) 0.0029 (9) 0.0022 (9)
C6 0.0148 (11) 0.0150 (12) 0.0190 (11) 0.0017 (9) 0.0021 (9) 0.0011 (9)
C7 0.0152 (11) 0.0147 (11) 0.0184 (11) 0.0035 (9) 0.0015 (9) 0.0019 (9)
C8 0.0188 (12) 0.0164 (12) 0.0158 (11) 0.0053 (10) 0.0017 (9) 0.0003 (9)
C9 0.0272 (13) 0.0139 (11) 0.0122 (10) 0.0025 (10) −0.0002 (9) 0.0008 (8)
C10 0.0229 (13) 0.0174 (12) 0.0215 (11) 0.0047 (10) −0.0008 (10) −0.0017 (9)
C11 0.0295 (14) 0.0235 (14) 0.0187 (11) 0.0014 (11) 0.0096 (10) −0.0013 (10)
C12 0.0417 (16) 0.0206 (13) 0.0130 (11) 0.0006 (11) 0.0019 (11) 0.0039 (9)
C13 0.0313 (14) 0.0260 (14) 0.0192 (12) 0.0095 (11) −0.0024 (10) 0.0043 (10)
C14 0.0255 (13) 0.0202 (13) 0.0188 (11) 0.0057 (10) 0.0048 (10) 0.0022 (9)
C15 0.0168 (11) 0.0150 (12) 0.0182 (11) 0.0039 (9) 0.0013 (9) 0.0024 (9)
C16 0.0144 (11) 0.0167 (12) 0.0149 (10) 0.0025 (9) 0.0007 (9) 0.0005 (9)
C17 0.0165 (12) 0.0133 (11) 0.0202 (11) 0.0020 (9) 0.0026 (9) 0.0019 (9)
C18 0.0154 (11) 0.0173 (12) 0.0192 (11) 0.0029 (9) 0.0015 (9) 0.0050 (9)
C19 0.0165 (11) 0.0203 (12) 0.0140 (10) 0.0015 (9) 0.0019 (9) 0.0027 (9)
C20 0.0123 (11) 0.0151 (12) 0.0184 (11) 0.0013 (9) 0.0009 (9) 0.0004 (9)
C21 0.0178 (12) 0.0134 (11) 0.0158 (10) 0.0040 (9) 0.0018 (9) 0.0014 (8)
C22 0.0192 (12) 0.0150 (12) 0.0162 (10) 0.0031 (9) 0.0014 (9) 0.0004 (9)
C23 0.0279 (13) 0.0156 (12) 0.0137 (10) 0.0064 (10) −0.0008 (10) 0.0015 (9)
C24 0.0251 (13) 0.0168 (12) 0.0210 (11) 0.0028 (10) 0.0032 (10) 0.0034 (9)
C25 0.0273 (14) 0.0239 (14) 0.0238 (12) 0.0047 (11) −0.0077 (11) 0.0006 (10)
C26 0.0438 (17) 0.0286 (15) 0.0164 (11) 0.0093 (13) −0.0042 (11) 0.0055 (10)
C27 0.0409 (16) 0.0349 (16) 0.0209 (12) 0.0054 (13) 0.0058 (12) 0.0112 (11)
C28 0.0300 (14) 0.0258 (14) 0.0197 (12) 0.0021 (11) 0.0016 (10) 0.0030 (10)

Geometric parameters (Å, °)

Cl1—C3 1.719 (2) C4—C5 1.401 (3)
Cl2—C4 1.714 (2) C5—C6 1.401 (3)
Cl3—C5 1.714 (2) C6—C7 1.382 (3)
Cl4—C6 1.722 (2) C7—C8 1.503 (3)
Cl5—C17 1.718 (2) C9—C10 1.375 (3)
Cl6—C18 1.717 (2) C9—C14 1.381 (3)
Cl7—C19 1.715 (2) C10—C11 1.380 (3)
Cl8—C20 1.725 (2) C11—C12 1.373 (3)
F1—C10 1.344 (2) C12—C13 1.370 (3)
F2—C11 1.344 (2) C13—C14 1.388 (3)
F3—C12 1.350 (2) C13—H13 0.9500
F4—C24 1.337 (2) C14—H14 0.9500
F5—C25 1.341 (3) C15—C16 1.499 (3)
F6—C26 1.347 (2) C16—C17 1.382 (3)
O1—C1 1.196 (2) C16—C21 1.387 (3)
O2—C8 1.194 (2) C17—C18 1.408 (3)
O3—C15 1.197 (2) C18—C19 1.398 (3)
O4—C22 1.195 (2) C19—C20 1.404 (3)
N1—C1 1.399 (3) C20—C21 1.380 (3)
N1—C8 1.409 (2) C21—C22 1.501 (3)
N1—C9 1.427 (2) C23—C28 1.371 (3)
N2—C22 1.402 (2) C23—C24 1.378 (3)
N2—C15 1.407 (3) C24—C25 1.389 (3)
N2—C23 1.430 (2) C25—C26 1.366 (3)
C1—C2 1.500 (3) C26—C27 1.374 (3)
C2—C3 1.376 (3) C27—C28 1.393 (3)
C2—C7 1.387 (3) C27—H27 0.9500
C3—C4 1.404 (3) C28—H28 0.9500
C1—N1—C8 113.57 (17) C9—C14—C13 120.1 (2)
C1—N1—C9 123.83 (18) C9—C14—H14 120.0
C8—N1—C9 122.60 (18) C13—C14—H14 120.0
C22—N2—C15 113.18 (17) O3—C15—N2 125.24 (19)
C22—N2—C23 123.55 (18) O3—C15—C16 130.1 (2)
C15—N2—C23 123.13 (18) N2—C15—C16 104.68 (17)
O1—C1—N1 125.92 (19) C17—C16—C21 121.68 (19)
O1—C1—C2 129.4 (2) C17—C16—C15 129.5 (2)
N1—C1—C2 104.68 (17) C21—C16—C15 108.75 (18)
C3—C2—C7 121.54 (19) C16—C17—C18 117.6 (2)
C3—C2—C1 129.7 (2) C16—C17—Cl5 121.73 (16)
C7—C2—C1 108.72 (18) C18—C17—Cl5 120.65 (16)
C2—C3—C4 117.8 (2) C19—C18—C17 120.79 (19)
C2—C3—Cl1 121.46 (17) C19—C18—Cl6 119.63 (16)
C4—C3—Cl1 120.77 (16) C17—C18—Cl6 119.54 (17)
C5—C4—C3 120.72 (19) C18—C19—C20 120.45 (19)
C5—C4—Cl2 119.49 (16) C18—C19—Cl7 119.97 (16)
C3—C4—Cl2 119.79 (17) C20—C19—Cl7 119.56 (17)
C4—C5—C6 120.68 (19) C21—C20—C19 118.1 (2)
C4—C5—Cl3 120.40 (16) C21—C20—Cl8 120.78 (16)
C6—C5—Cl3 118.92 (17) C19—C20—Cl8 121.09 (16)
C7—C6—C5 117.6 (2) C20—C21—C16 121.3 (2)
C7—C6—Cl4 121.10 (17) C20—C21—C22 130.2 (2)
C5—C6—Cl4 121.33 (17) C16—C21—C22 108.44 (18)
C6—C7—C2 121.7 (2) O4—C22—N2 125.79 (19)
C6—C7—C8 129.7 (2) O4—C22—C21 129.3 (2)
C2—C7—C8 108.60 (18) N2—C22—C21 104.91 (18)
O2—C8—N1 125.93 (19) C28—C23—C24 120.4 (2)
O2—C8—C7 129.7 (2) C28—C23—N2 121.9 (2)
N1—C8—C7 104.38 (18) C24—C23—N2 117.7 (2)
C10—C9—C14 120.17 (19) F4—C24—C23 120.94 (19)
C10—C9—N1 119.27 (19) F4—C24—C25 119.1 (2)
C14—C9—N1 120.53 (19) C23—C24—C25 120.0 (2)
F1—C10—C9 120.85 (19) F5—C25—C26 121.5 (2)
F1—C10—C11 119.0 (2) F5—C25—C24 119.6 (2)
C9—C10—C11 120.2 (2) C26—C25—C24 118.9 (2)
F2—C11—C12 120.8 (2) F6—C26—C25 118.4 (2)
F2—C11—C10 120.3 (2) F6—C26—C27 119.6 (2)
C12—C11—C10 118.9 (2) C25—C26—C27 122.0 (2)
F3—C12—C13 120.3 (2) C26—C27—C28 118.6 (2)
F3—C12—C11 117.7 (2) C26—C27—H27 120.7
C13—C12—C11 122.0 (2) C28—C27—H27 120.7
C12—C13—C14 118.6 (2) C23—C28—C27 120.0 (2)
C12—C13—H13 120.7 C23—C28—H28 120.0
C14—C13—H13 120.7 C27—C28—H28 120.0
C8—N1—C1—O1 −179.0 (2) C22—N2—C15—O3 −178.8 (2)
C9—N1—C1—O1 1.9 (4) C23—N2—C15—O3 −3.1 (4)
C8—N1—C1—C2 0.2 (2) C22—N2—C15—C16 −0.4 (2)
C9—N1—C1—C2 −178.89 (19) C23—N2—C15—C16 175.38 (19)
O1—C1—C2—C3 −2.9 (4) O3—C15—C16—C17 −0.1 (4)
N1—C1—C2—C3 177.9 (2) N2—C15—C16—C17 −178.4 (2)
O1—C1—C2—C7 177.5 (2) O3—C15—C16—C21 177.4 (2)
N1—C1—C2—C7 −1.7 (2) N2—C15—C16—C21 −0.9 (2)
C7—C2—C3—C4 −1.4 (3) C21—C16—C17—C18 −2.9 (3)
C1—C2—C3—C4 179.1 (2) C15—C16—C17—C18 174.3 (2)
C7—C2—C3—Cl1 179.12 (16) C21—C16—C17—Cl5 178.95 (16)
C1—C2—C3—Cl1 −0.4 (3) C15—C16—C17—Cl5 −3.8 (3)
C2—C3—C4—C5 0.1 (3) C16—C17—C18—C19 1.3 (3)
Cl1—C3—C4—C5 179.60 (16) Cl5—C17—C18—C19 179.47 (16)
C2—C3—C4—Cl2 −179.57 (16) C16—C17—C18—Cl6 −176.17 (16)
Cl1—C3—C4—Cl2 −0.1 (3) Cl5—C17—C18—Cl6 2.0 (3)
C3—C4—C5—C6 1.2 (3) C17—C18—C19—C20 1.2 (3)
Cl2—C4—C5—C6 −179.15 (16) Cl6—C18—C19—C20 178.69 (16)
C3—C4—C5—Cl3 −178.42 (16) C17—C18—C19—Cl7 −177.29 (16)
Cl2—C4—C5—Cl3 1.3 (3) Cl6—C18—C19—Cl7 0.2 (3)
C4—C5—C6—C7 −1.1 (3) C18—C19—C20—C21 −2.1 (3)
Cl3—C5—C6—C7 178.44 (15) Cl7—C19—C20—C21 176.36 (16)
C4—C5—C6—Cl4 178.15 (16) C18—C19—C20—Cl8 179.31 (16)
Cl3—C5—C6—Cl4 −2.3 (3) Cl7—C19—C20—Cl8 −2.2 (3)
C5—C6—C7—C2 −0.1 (3) C19—C20—C21—C16 0.6 (3)
Cl4—C6—C7—C2 −179.42 (16) Cl8—C20—C21—C16 179.13 (16)
C5—C6—C7—C8 178.2 (2) C19—C20—C21—C22 −176.3 (2)
Cl4—C6—C7—C8 −1.1 (3) Cl8—C20—C21—C22 2.2 (3)
C3—C2—C7—C6 1.4 (3) C17—C16—C21—C20 2.0 (3)
C1—C2—C7—C6 −178.94 (19) C15—C16—C21—C20 −175.73 (19)
C3—C2—C7—C8 −177.2 (2) C17—C16—C21—C22 179.53 (19)
C1—C2—C7—C8 2.4 (2) C15—C16—C21—C22 1.8 (2)
C1—N1—C8—O2 −178.4 (2) C15—N2—C22—O4 −179.2 (2)
C9—N1—C8—O2 0.8 (4) C23—N2—C22—O4 5.1 (4)
C1—N1—C8—C7 1.1 (2) C15—N2—C22—C21 1.4 (2)
C9—N1—C8—C7 −179.71 (18) C23—N2—C22—C21 −174.33 (19)
C6—C7—C8—O2 −1.2 (4) C20—C21—C22—O4 −4.1 (4)
C2—C7—C8—O2 177.3 (2) C16—C21—C22—O4 178.7 (2)
C6—C7—C8—N1 179.3 (2) C20—C21—C22—N2 175.3 (2)
C2—C7—C8—N1 −2.2 (2) C16—C21—C22—N2 −2.0 (2)
C1—N1—C9—C10 66.6 (3) C22—N2—C23—C28 −72.5 (3)
C8—N1—C9—C10 −112.4 (2) C15—N2—C23—C28 112.2 (3)
C1—N1—C9—C14 −115.1 (2) C22—N2—C23—C24 107.1 (2)
C8—N1—C9—C14 65.9 (3) C15—N2—C23—C24 −68.2 (3)
C14—C9—C10—F1 178.6 (2) C28—C23—C24—F4 −179.3 (2)
N1—C9—C10—F1 −3.1 (3) N2—C23—C24—F4 1.1 (3)
C14—C9—C10—C11 −2.1 (4) C28—C23—C24—C25 0.2 (3)
N1—C9—C10—C11 176.2 (2) N2—C23—C24—C25 −179.4 (2)
F1—C10—C11—F2 −0.2 (4) F4—C24—C25—F5 −1.6 (3)
C9—C10—C11—F2 −179.5 (2) C23—C24—C25—F5 178.8 (2)
F1—C10—C11—C12 −179.9 (2) F4—C24—C25—C26 179.4 (2)
C9—C10—C11—C12 0.8 (4) C23—C24—C25—C26 −0.1 (4)
F2—C11—C12—F3 0.4 (4) F5—C25—C26—F6 1.8 (4)
C10—C11—C12—F3 −179.8 (2) C24—C25—C26—F6 −179.3 (2)
F2—C11—C12—C13 −179.0 (2) F5—C25—C26—C27 −178.8 (2)
C10—C11—C12—C13 0.7 (4) C24—C25—C26—C27 0.1 (4)
F3—C12—C13—C14 179.7 (2) F6—C26—C27—C28 179.2 (2)
C11—C12—C13—C14 −0.9 (4) C25—C26—C27—C28 −0.2 (4)
C10—C9—C14—C13 2.0 (4) C24—C23—C28—C27 −0.3 (3)
N1—C9—C14—C13 −176.3 (2) N2—C23—C28—C27 179.3 (2)
C12—C13—C14—C9 −0.5 (4) C26—C27—C28—C23 0.3 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C14—H14···O3i 0.95 2.44 3.210 (3) 138.
C27—H27···F3ii 0.95 2.45 3.379 (3) 165.
C28—H28···O1 0.95 2.50 3.403 (3) 158.

Symmetry codes: (i) x, y−1, z; (ii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5228).

References

  1. Barchin, B. M., Cuadro, A. M. & Alvarez-Builla, J. (2002). Synlett, 2, 343–345.
  2. Bruker (2001). SADABS Bruker AXS Inc., Madison, Wiscosin, USA.
  3. Bruker (2007). SMART and SAINT Bruker AXS Inc., Madison, Wiscosin, USA.
  4. Fu, X.-S., Yu, X.-P., Wang, W.-M. & Lin, F. (2010a). Acta Cryst. E66, o1809.
  5. Fu, X.-S., Yu, X.-P., Wang, W.-M. & Lin, F. (2010b). Acta Cryst. E66, o1744.
  6. Fu, X.-S., Yu, X.-P., Wang, W.-M. & Lin, F. (2010c). Acta Cryst. E66, o1859.
  7. Han, K. J. & Kay, K. Y. (2005). J. Korean Chem. Soc. 49, 233–238.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Valkonen, A., Lahtinen, T. & Rissanen, K. (2007). Acta Cryst. E63, o472–o473.
  10. Xu, D., Shi, Y.-Q., Chen, B., Cheng, Y.-H. & Gao, X. (2006). Acta Cryst. E62, o408–o409.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811020721/xu5228sup1.cif

e-67-o1604-sup1.cif (25.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811020721/xu5228Isup2.hkl

e-67-o1604-Isup2.hkl (327.1KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811020721/xu5228Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES