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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jun 30;66(Pt 7):o1859. doi: 10.1107/S1600536810024177

N-(2,3,4-Trifluoro­phen­yl)phthalimide

Xian-Shu Fu a, Xiao-Ping Yu a, Wei-Min Wang a,*, Fang Lin a
PMCID: PMC3006749  PMID: 21588056

Abstract

In the title compound, C14H6F3NO2, the benzene ring and the phthalimide ring system make a dihedral angle of 60.12 (7)°. Weak inter­molecular C—H⋯O and C—H⋯F hydrogen bonds are present in the crystal structure.

Related literature

The title compound is a key inter­mediate in the synthesis 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. (2010).graphic file with name e-66-o1859-scheme1.jpg

Experimental

Crystal data

  • C14H6F3NO2

  • M r = 277.20

  • Monoclinic, Inline graphic

  • a = 6.8422 (14) Å

  • b = 21.082 (4) Å

  • c = 7.9727 (16) Å

  • β = 101.98 (3)°

  • V = 1125.0 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.14 mm−1

  • T = 113 K

  • 0.20 × 0.18 × 0.12 mm

Data collection

  • Rigaku Saturn CCD area-detector diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) T min = 0.972, T max = 0.983

  • 8049 measured reflections

  • 1980 independent reflections

  • 1603 reflections with I > 2σ(I)

  • R int = 0.034

Refinement

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.094

  • S = 1.03

  • 1980 reflections

  • 182 parameters

  • H-atom parameters constrained

  • Δρmax = 0.34 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810024177/ng2787sup1.cif

e-66-o1859-sup1.cif (17.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810024177/ng2787Isup2.hkl

e-66-o1859-Isup2.hkl (97.4KB, hkl)

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
C4—H4⋯O2i 0.95 2.55 3.1855 (18) 124
C10—H10⋯F1ii 0.95 2.54 3.3647 (18) 145
C11—H11⋯O1iii 0.95 2.55 3.428 (2) 154

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

Acknowledgments

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).

supplementary crystallographic information

Comment

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, 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 60.12 (7) °, which is similar to 59.95 (4) ° found in a related compound N-(2-fluorophenyl)phthalimide (Xu et al. 2006). Weak intermolecular C—H···O and C—H···F hydrogen bonding are present in the crystal structure (Table 1).

Experimental

An acetic acid solution of phthalic anhydride (14.8 g, 100 mmol) and 2,3,4-trifluoroaniline (10.55 ml, 100 mmol) was refluxed overnight, and then filtered. The crude product was recrystallized from ethyl acetate.

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

C14H6F3NO2 F(000) = 560
Mr = 277.20 Dx = 1.637 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 3644 reflections
a = 6.8422 (14) Å θ = 1.9–27.8°
b = 21.082 (4) Å µ = 0.14 mm1
c = 7.9727 (16) Å T = 113 K
β = 101.98 (3)° Prism, colorless
V = 1125.0 (4) Å3 0.20 × 0.18 × 0.12 mm
Z = 4

Data collection

Rigaku Saturn CCD area-detector diffractometer 1980 independent reflections
Radiation source: rotating anode 1603 reflections with I > 2σ(I)
confocal Rint = 0.034
Detector resolution: 7.31 pixels mm-1 θmax = 25.0°, θmin = 1.9°
ω and φ scans h = −8→8
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −24→25
Tmin = 0.972, Tmax = 0.983 l = −7→9
8049 measured reflections

Refinement

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)] = 0.034 H-atom parameters constrained
wR(F2) = 0.094 w = 1/[σ2(Fo2) + (0.0663P)2] where P = (Fo2 + 2Fc2)/3
S = 1.03 (Δ/σ)max = 0.002
1980 reflections Δρmax = 0.34 e Å3
182 parameters Δρmin = −0.21 e Å3
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: 0.097 (6)

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
F1 0.36805 (13) 0.27803 (5) 1.30697 (12) 0.0324 (3)
F2 0.04277 (12) 0.20200 (5) 1.25161 (11) 0.0286 (3)
F3 0.00346 (11) 0.10870 (4) 1.01757 (10) 0.0245 (3)
O1 0.29321 (15) 0.14544 (5) 0.58108 (12) 0.0246 (3)
O2 0.28164 (15) 0.00092 (5) 1.01024 (12) 0.0228 (3)
N1 0.28999 (17) 0.08556 (6) 0.82561 (14) 0.0181 (3)
C1 0.28328 (19) 0.09456 (7) 0.64828 (17) 0.0176 (3)
C2 0.26306 (18) 0.02990 (7) 0.57338 (17) 0.0162 (3)
C3 0.2489 (2) 0.01067 (7) 0.40531 (18) 0.0193 (4)
H3 0.2475 0.0406 0.3160 0.023*
C4 0.23668 (19) −0.05431 (8) 0.37222 (18) 0.0214 (4)
H4 0.2272 −0.0690 0.2582 0.026*
C5 0.2381 (2) −0.09816 (8) 0.50331 (18) 0.0231 (4)
H5 0.2302 −0.1422 0.4771 0.028*
C6 0.2507 (2) −0.07859 (7) 0.67177 (18) 0.0200 (3)
H6 0.2510 −0.1083 0.7613 0.024*
C7 0.26293 (18) −0.01410 (7) 0.70366 (16) 0.0161 (3)
C8 0.27847 (19) 0.02073 (7) 0.86743 (17) 0.0168 (3)
C9 0.31396 (19) 0.13524 (7) 0.94859 (17) 0.0175 (3)
C10 0.4794 (2) 0.17526 (7) 0.97522 (18) 0.0216 (4)
H10 0.5796 0.1693 0.9102 0.026*
C11 0.4998 (2) 0.22367 (8) 1.09549 (19) 0.0240 (4)
H11 0.6125 0.2510 1.1129 0.029*
C12 0.3538 (2) 0.23125 (7) 1.18896 (18) 0.0225 (4)
C13 0.1879 (2) 0.19236 (8) 1.16429 (18) 0.0207 (4)
C14 0.16934 (19) 0.14500 (7) 1.04425 (17) 0.0181 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.0371 (5) 0.0252 (6) 0.0336 (5) −0.0042 (4) 0.0044 (4) −0.0152 (4)
F2 0.0289 (5) 0.0319 (6) 0.0280 (5) 0.0003 (4) 0.0132 (4) −0.0096 (4)
F3 0.0213 (5) 0.0273 (6) 0.0262 (5) −0.0077 (4) 0.0080 (3) −0.0059 (4)
O1 0.0342 (6) 0.0189 (7) 0.0220 (6) 0.0039 (5) 0.0086 (4) 0.0058 (4)
O2 0.0300 (6) 0.0236 (7) 0.0159 (5) −0.0026 (4) 0.0072 (4) 0.0024 (4)
N1 0.0239 (6) 0.0158 (7) 0.0156 (6) −0.0014 (5) 0.0062 (5) −0.0003 (5)
C1 0.0159 (7) 0.0224 (9) 0.0150 (7) 0.0029 (6) 0.0044 (6) 0.0032 (6)
C2 0.0126 (6) 0.0191 (9) 0.0172 (7) 0.0018 (6) 0.0039 (5) 0.0014 (6)
C3 0.0164 (7) 0.0271 (10) 0.0145 (7) 0.0022 (6) 0.0030 (5) 0.0015 (6)
C4 0.0175 (7) 0.0288 (10) 0.0177 (7) 0.0014 (6) 0.0029 (6) −0.0041 (6)
C5 0.0228 (8) 0.0215 (9) 0.0253 (8) −0.0002 (6) 0.0053 (6) −0.0065 (6)
C6 0.0210 (7) 0.0184 (9) 0.0209 (8) 0.0001 (6) 0.0047 (6) 0.0006 (6)
C7 0.0139 (7) 0.0190 (9) 0.0157 (7) 0.0007 (6) 0.0035 (5) −0.0001 (5)
C8 0.0157 (7) 0.0179 (9) 0.0176 (7) 0.0003 (6) 0.0051 (5) 0.0010 (6)
C9 0.0216 (7) 0.0165 (9) 0.0141 (7) 0.0006 (6) 0.0027 (6) 0.0007 (6)
C10 0.0222 (7) 0.0198 (9) 0.0242 (8) −0.0010 (6) 0.0076 (6) 0.0027 (6)
C11 0.0229 (8) 0.0199 (9) 0.0280 (8) −0.0045 (6) 0.0025 (6) 0.0012 (6)
C12 0.0285 (8) 0.0165 (9) 0.0200 (7) 0.0011 (6) −0.0003 (6) −0.0041 (6)
C13 0.0215 (7) 0.0233 (9) 0.0181 (7) 0.0027 (6) 0.0058 (6) 0.0008 (6)
C14 0.0172 (7) 0.0180 (9) 0.0179 (7) −0.0029 (6) 0.0011 (6) 0.0005 (6)

Geometric parameters (Å, °)

F1—C12 1.3525 (17) C4—H4 0.9500
F2—C13 1.3411 (17) C5—C6 1.390 (2)
F3—C14 1.3486 (16) C5—H5 0.9500
O1—C1 1.2072 (18) C6—C7 1.382 (2)
O2—C8 1.2087 (16) C6—H6 0.9500
N1—C8 1.4129 (19) C7—C8 1.4824 (19)
N1—C1 1.4178 (17) C9—C14 1.384 (2)
N1—C9 1.4207 (18) C9—C10 1.392 (2)
C1—C2 1.483 (2) C10—C11 1.387 (2)
C2—C3 1.3840 (19) C10—H10 0.9500
C2—C7 1.3927 (19) C11—C12 1.374 (2)
C3—C4 1.394 (2) C11—H11 0.9500
C3—H3 0.9500 C12—C13 1.381 (2)
C4—C5 1.394 (2) C13—C14 1.371 (2)
C8—N1—C1 111.90 (11) C2—C7—C8 108.41 (13)
C8—N1—C9 123.66 (11) O2—C8—N1 124.44 (13)
C1—N1—C9 124.39 (12) O2—C8—C7 129.98 (14)
O1—C1—N1 124.63 (13) N1—C8—C7 105.58 (11)
O1—C1—C2 130.33 (13) C14—C9—C10 118.52 (13)
N1—C1—C2 105.04 (12) C14—C9—N1 119.76 (12)
C3—C2—C7 121.07 (14) C10—C9—N1 121.72 (12)
C3—C2—C1 129.87 (13) C11—C10—C9 120.87 (13)
C7—C2—C1 109.05 (12) C11—C10—H10 119.6
C2—C3—C4 117.42 (13) C9—C10—H10 119.6
C2—C3—H3 121.3 C12—C11—C10 118.70 (14)
C4—C3—H3 121.3 C12—C11—H11 120.7
C5—C4—C3 121.26 (14) C10—C11—H11 120.7
C5—C4—H4 119.4 F1—C12—C11 120.43 (13)
C3—C4—H4 119.4 F1—C12—C13 118.06 (13)
C6—C5—C4 121.12 (15) C11—C12—C13 121.50 (14)
C6—C5—H5 119.5 F2—C13—C14 120.11 (13)
C4—C5—H5 119.5 F2—C13—C12 120.76 (13)
C7—C6—C5 117.30 (14) C14—C13—C12 119.08 (13)
C7—C6—H6 121.3 F3—C14—C13 118.45 (12)
C5—C6—H6 121.3 F3—C14—C9 120.21 (12)
C6—C7—C2 121.82 (13) C13—C14—C9 121.32 (13)
C6—C7—C8 129.77 (13)
C8—N1—C1—O1 −179.01 (13) C2—C7—C8—O2 179.32 (13)
C9—N1—C1—O1 −1.5 (2) C6—C7—C8—N1 178.93 (13)
C8—N1—C1—C2 0.83 (14) C2—C7—C8—N1 −0.75 (14)
C9—N1—C1—C2 178.32 (11) C8—N1—C9—C14 −61.69 (18)
O1—C1—C2—C3 −0.5 (2) C1—N1—C9—C14 121.12 (15)
N1—C1—C2—C3 179.72 (13) C8—N1—C9—C10 118.90 (15)
O1—C1—C2—C7 178.52 (14) C1—N1—C9—C10 −58.29 (18)
N1—C1—C2—C7 −1.30 (14) C14—C9—C10—C11 0.3 (2)
C7—C2—C3—C4 −0.67 (19) N1—C9—C10—C11 179.76 (13)
C1—C2—C3—C4 178.21 (12) C9—C10—C11—C12 0.3 (2)
C2—C3—C4—C5 0.2 (2) C10—C11—C12—F1 −179.77 (13)
C3—C4—C5—C6 0.3 (2) C10—C11—C12—C13 −0.7 (2)
C4—C5—C6—C7 −0.34 (19) F1—C12—C13—F2 1.9 (2)
C5—C6—C7—C2 −0.13 (19) C11—C12—C13—F2 −177.27 (13)
C5—C6—C7—C8 −179.77 (13) F1—C12—C13—C14 179.41 (13)
C3—C2—C7—C6 0.7 (2) C11—C12—C13—C14 0.3 (2)
C1—C2—C7—C6 −178.43 (12) F2—C13—C14—F3 −0.3 (2)
C3—C2—C7—C8 −179.64 (11) C12—C13—C14—F3 −177.88 (12)
C1—C2—C7—C8 1.28 (14) F2—C13—C14—C9 178.01 (12)
C1—N1—C8—O2 179.85 (12) C12—C13—C14—C9 0.4 (2)
C9—N1—C8—O2 2.3 (2) C10—C9—C14—F3 177.54 (12)
C1—N1—C8—C7 −0.09 (14) N1—C9—C14—F3 −1.9 (2)
C9—N1—C8—C7 −177.60 (11) C10—C9—C14—C13 −0.7 (2)
C6—C7—C8—O2 −1.0 (2) N1—C9—C14—C13 179.83 (13)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C4—H4···O2i 0.95 2.55 3.1855 (18) 124
C10—H10···F1ii 0.95 2.54 3.3647 (18) 145
C11—H11···O1iii 0.95 2.55 3.428 (2) 154

Symmetry codes: (i) x, y, z−1; (ii) x+1/2, −y+1/2, z−1/2; (iii) x+1/2, −y+1/2, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2787).

References

  1. Barchin, B. M., Cuadro, A. M. & Alvarez-Builla, J. (2002). Synlett, 2, 343–345.
  2. Fu, X.-S., Yu, X.-P., Wang, W.-M. & Lin, F. (2010). Acta Cryst. E66, o1744. [DOI] [PMC free article] [PubMed]
  3. Han, K. J. & Kay, K. Y. (2005). J. Korean Chem. Soc.49, 233–238.
  4. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Valkonen, A., Lahtinen, T. & Rissanen, K. (2007). Acta Cryst. E63, o472–o473.
  7. 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 datablocks I, global. DOI: 10.1107/S1600536810024177/ng2787sup1.cif

e-66-o1859-sup1.cif (17.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810024177/ng2787Isup2.hkl

e-66-o1859-Isup2.hkl (97.4KB, hkl)

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


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