organic compounds
4,5,6,7-Tetrachloro-2-(4-fluorophenyl)isoindoline-1,3-dione
aCollege of Life Sciences, China Jiliang University, Hangzhou 310018, People's Republic of China
*Correspondence e-mail: clshangzhou@yahoo.com.cn
The title compound, C14H4Cl4FNO2, has crystallographic twofold symmetry with the N and F atoms and two C atoms of the benzene ring located on a twofold rotation axis. The isoindoledione ring system is almost planar [maximum atomic deviation = 0.036 (3) Å], and is twisted with respect to the florobenzene ring, making a dihedral angle of 58.56 (16)°. Weak intermolecular C—H⋯Cl hydrogen bonding is present in the crystal structure.
Related literature
The title compound is an intermediate in the synthesis of organic electro-luminescent materials, see: Han & Kay (2005). For a related structure, see: Xu et al. (2006).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku/MSC, 2001); cell CrystalClear; data reduction: CrystalStructure (Rigaku/MSC, 2004); 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: SHELXL97.
Supporting information
10.1107/S1600536810023032/xu2780sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810023032/xu2780Isup2.hkl
An acetic acid solution of tetrachlorophthalic anhydride (28.6 g, 100 mmol) and 4-fluoroaniline (9.45 ml, 100 mmol) was refluxed overnight, and then filtered. The crude produce was recrystallized from ethyl acetate.
H atoms were positioned geometrically and refined as riding with C—H = 0.95 Å, and Uiso(H) = 1.2Ueq(C).
Data collection: CrystalClear (Rigaku/MSC, 2001); cell
CrystalClear (Rigaku/MSC, 2001); data reduction: CrystalStructure (Rigaku/MSC, 2004); 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: SHELXL97 (Sheldrick, 2008).Fig. 1. View of the molecule of showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. |
C14H4Cl4FNO2 | F(000) = 752 |
Mr = 378.98 | Dx = 1.896 Mg m−3 |
Orthorhombic, Pcca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2a 2ac | Cell parameters from 3007 reflections |
a = 7.9400 (16) Å | θ = 2.8–27.9° |
b = 5.6744 (11) Å | µ = 0.91 mm−1 |
c = 29.461 (6) Å | T = 113 K |
V = 1327.4 (5) Å3 | Prism, colorless |
Z = 4 | 0.20 × 0.18 × 0.12 mm |
Rigaku Saturn CCD area-detector diffractometer | 1174 independent reflections |
Radiation source: rotating anode | 1053 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.039 |
Detector resolution: 7.31 pixels mm-1 | θmax = 25.0°, θmin = 2.8° |
ω and ϕ scans | h = −9→9 |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2001) | k = −6→6 |
Tmin = 0.839, Tmax = 0.899 | l = −35→30 |
6423 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.050 | H-atom parameters constrained |
wR(F2) = 0.204 | w = 1/[σ2(Fo2) + (0.1623P)2 + 2.0637P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.001 |
1174 reflections | Δρmax = 0.84 e Å−3 |
103 parameters | Δρmin = −0.74 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.039 (8) |
C14H4Cl4FNO2 | V = 1327.4 (5) Å3 |
Mr = 378.98 | Z = 4 |
Orthorhombic, Pcca | Mo Kα radiation |
a = 7.9400 (16) Å | µ = 0.91 mm−1 |
b = 5.6744 (11) Å | T = 113 K |
c = 29.461 (6) Å | 0.20 × 0.18 × 0.12 mm |
Rigaku Saturn CCD area-detector diffractometer | 1174 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2001) | 1053 reflections with I > 2σ(I) |
Tmin = 0.839, Tmax = 0.899 | Rint = 0.039 |
6423 measured reflections |
R[F2 > 2σ(F2)] = 0.050 | 0 restraints |
wR(F2) = 0.204 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.84 e Å−3 |
1174 reflections | Δρmin = −0.74 e Å−3 |
103 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cl1 | 0.14081 (12) | 0.27246 (16) | −0.00242 (3) | 0.0266 (5) | |
Cl2 | 0.01306 (11) | 0.05859 (15) | 0.08874 (3) | 0.0246 (5) | |
F1 | 0.2500 | 0.5000 | 0.39104 (10) | 0.0445 (10) | |
O1 | 0.0906 (3) | 0.1621 (5) | 0.19160 (8) | 0.0236 (7) | |
N1 | 0.2500 | 0.5000 | 0.20376 (13) | 0.0224 (10) | |
C1 | 0.1999 (4) | 0.4011 (6) | 0.04757 (10) | 0.0199 (8) | |
C2 | 0.1431 (4) | 0.3007 (7) | 0.08894 (12) | 0.0209 (9) | |
C3 | 0.1986 (4) | 0.4021 (6) | 0.12895 (12) | 0.0184 (8) | |
C4 | 0.1677 (4) | 0.3289 (6) | 0.17733 (11) | 0.0183 (8) | |
C5 | 0.2500 | 0.5000 | 0.25202 (14) | 0.0173 (11) | |
C6 | 0.1893 (4) | 0.6957 (6) | 0.27533 (11) | 0.0206 (8) | |
H6 | 0.1499 | 0.8293 | 0.2591 | 0.025* | |
C7 | 0.1864 (5) | 0.6948 (7) | 0.32247 (12) | 0.0264 (9) | |
H7 | 0.1419 | 0.8248 | 0.3389 | 0.032* | |
C8 | 0.2500 | 0.5000 | 0.34501 (17) | 0.0338 (14) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0358 (8) | 0.0274 (8) | 0.0165 (7) | 0.0042 (4) | −0.0031 (3) | −0.0059 (3) |
Cl2 | 0.0301 (7) | 0.0219 (8) | 0.0219 (7) | −0.0043 (3) | −0.0010 (3) | −0.0042 (3) |
F1 | 0.063 (2) | 0.054 (2) | 0.0166 (17) | −0.027 (2) | 0.000 | 0.000 |
O1 | 0.0269 (14) | 0.0221 (14) | 0.0218 (13) | −0.0051 (10) | 0.0023 (10) | 0.0039 (10) |
N1 | 0.032 (2) | 0.017 (2) | 0.017 (2) | −0.0042 (18) | 0.000 | 0.000 |
C1 | 0.0228 (18) | 0.0250 (18) | 0.0119 (17) | 0.0079 (13) | −0.0016 (11) | −0.0046 (12) |
C2 | 0.0182 (16) | 0.0226 (19) | 0.022 (2) | 0.0011 (13) | 0.0021 (11) | 0.0000 (14) |
C3 | 0.0179 (16) | 0.0204 (16) | 0.0168 (17) | 0.0031 (13) | −0.0014 (12) | −0.0001 (13) |
C4 | 0.0159 (14) | 0.0220 (19) | 0.0171 (18) | 0.0024 (14) | −0.0009 (12) | 0.0013 (13) |
C5 | 0.014 (2) | 0.020 (2) | 0.018 (2) | −0.0002 (18) | 0.000 | 0.000 |
C6 | 0.0195 (16) | 0.0208 (18) | 0.0213 (18) | −0.0038 (13) | 0.0008 (12) | −0.0016 (14) |
C7 | 0.0243 (18) | 0.030 (2) | 0.0252 (19) | −0.0066 (15) | 0.0024 (14) | −0.0089 (15) |
C8 | 0.050 (3) | 0.036 (3) | 0.015 (2) | −0.025 (3) | 0.000 | 0.000 |
Cl1—C1 | 1.709 (3) | C3—C3i | 1.379 (7) |
Cl2—C2 | 1.719 (4) | C3—C4 | 1.504 (5) |
F1—C8 | 1.356 (6) | C5—C6 | 1.392 (4) |
O1—C4 | 1.203 (5) | C5—C6i | 1.392 (4) |
N1—C4 | 1.406 (4) | C6—C7 | 1.389 (5) |
N1—C4i | 1.406 (4) | C6—H6 | 0.9500 |
N1—C5 | 1.422 (5) | C7—C8 | 1.385 (5) |
C1—C1i | 1.376 (7) | C7—H7 | 0.9500 |
C1—C2 | 1.419 (5) | C8—C7i | 1.385 (5) |
C2—C3 | 1.384 (5) | ||
C4—N1—C4i | 112.7 (4) | N1—C4—C3 | 105.0 (3) |
C4—N1—C5 | 123.7 (2) | C6—C5—C6i | 120.9 (4) |
C4i—N1—C5 | 123.7 (2) | C6—C5—N1 | 119.6 (2) |
C1i—C1—C2 | 120.7 (2) | C6i—C5—N1 | 119.6 (2) |
C1i—C1—Cl1 | 120.48 (13) | C7—C6—C5 | 119.7 (3) |
C2—C1—Cl1 | 118.8 (3) | C7—C6—H6 | 120.1 |
C3—C2—C1 | 117.6 (3) | C5—C6—H6 | 120.1 |
C3—C2—Cl2 | 121.8 (3) | C8—C7—C6 | 118.4 (4) |
C1—C2—Cl2 | 120.6 (3) | C8—C7—H7 | 120.8 |
C3i—C3—C2 | 121.6 (2) | C6—C7—H7 | 120.8 |
C3i—C3—C4 | 108.58 (19) | F1—C8—C7i | 118.6 (2) |
C2—C3—C4 | 129.8 (3) | F1—C8—C7 | 118.6 (2) |
O1—C4—N1 | 125.9 (3) | C7i—C8—C7 | 122.7 (5) |
O1—C4—C3 | 129.1 (3) | ||
C1i—C1—C2—C3 | −3.0 (6) | C2—C3—C4—O1 | 1.9 (6) |
Cl1—C1—C2—C3 | 177.3 (2) | C3i—C3—C4—N1 | 3.1 (4) |
C1i—C1—C2—Cl2 | 178.1 (3) | C2—C3—C4—N1 | −178.2 (3) |
Cl1—C1—C2—Cl2 | −1.6 (4) | C4—N1—C5—C6 | −122.6 (2) |
C1—C2—C3—C3i | 1.9 (6) | C4i—N1—C5—C6 | 57.4 (2) |
Cl2—C2—C3—C3i | −179.2 (3) | C4—N1—C5—C6i | 57.4 (2) |
C1—C2—C3—C4 | −176.6 (3) | C4i—N1—C5—C6i | −122.6 (2) |
Cl2—C2—C3—C4 | 2.3 (5) | C6i—C5—C6—C7 | −1.1 (2) |
C4i—N1—C4—O1 | 178.8 (4) | N1—C5—C6—C7 | 178.9 (2) |
C5—N1—C4—O1 | −1.2 (4) | C5—C6—C7—C8 | 2.1 (4) |
C4i—N1—C4—C3 | −1.12 (15) | C6—C7—C8—F1 | 178.9 (2) |
C5—N1—C4—C3 | 178.88 (15) | C6—C7—C8—C7i | −1.1 (2) |
C3i—C3—C4—O1 | −176.8 (4) |
Symmetry code: (i) −x+1/2, −y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7···Cl2ii | 0.95 | 2.80 | 3.690 (4) | 157 |
Symmetry code: (ii) −x, y+1, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C14H4Cl4FNO2 |
Mr | 378.98 |
Crystal system, space group | Orthorhombic, Pcca |
Temperature (K) | 113 |
a, b, c (Å) | 7.9400 (16), 5.6744 (11), 29.461 (6) |
V (Å3) | 1327.4 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.91 |
Crystal size (mm) | 0.20 × 0.18 × 0.12 |
Data collection | |
Diffractometer | Rigaku Saturn CCD area-detector diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku/MSC, 2001) |
Tmin, Tmax | 0.839, 0.899 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6423, 1174, 1053 |
Rint | 0.039 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.050, 0.204, 1.04 |
No. of reflections | 1174 |
No. of parameters | 103 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.84, −0.74 |
Computer programs: CrystalClear (Rigaku/MSC, 2001), CrystalStructure (Rigaku/MSC, 2004), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C7—H7···Cl2i | 0.95 | 2.80 | 3.690 (4) | 157 |
Symmetry code: (i) −x, y+1, −z+1/2. |
Acknowledgements
The work was supported by the Major Research Program of Zhejiang Province (No. 2008 C02007–2) and the Zhejiang Provincial Natural Science Foundation of China (No. Y307128).
References
Han, K. J. & Kay, K. Y. (2005). J. Korean Chem. Soc. 49, 233–238. CAS Google Scholar
Rigaku/MSC (2001). CrystalClear. Rigaku/MSC, Tokyo, Japan. Google Scholar
Rigaku/MSC (2004). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Xu, D., Shi, Y.-Q., Chen, B., Cheng, Y.-H. & Gao, X. (2006). Acta Cryst. E62, o408–o409. Web of Science CSD CrossRef IUCr Journals Google Scholar
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The title compound is a key intermediate in the synthesis of organic electro-luminescent materials. The emission of light by organic molecules exposed to an electric field has been wide investigated in both an academic and industrial context (Han & Kay, 2005).
The molecular structure of the title compound is illustrated in Fig. 1. In the title compound, the dihedral angle between the benzene ring and the indole ring system is 58.56 (16)°, which is similar to 59.95 (4)° found in a related compound N-(2-fluorophenyl)phthalimide (Xu et al., 2006). Weak intermolecular C—H···Cl hydrogen bonding is present in the crystal structure (Table 1).