organic compounds
N,N-Dimethyl-4-[(E)-2-(3,6,7-tribromo-9-butyl-9H-carbazol-2-yl)ethenyl]aniline
aOrganic Materials Laboratory, Department of Chemistry, Indian Institute of Technology Roorkee, Roorkee 247 667, India, bDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, and cChemistry Department, Faculty of Science, King Abdulaziz University, PO Box 80203 Jeddah, Saudi Arabia
*Correspondence e-mail: edward.tiekink@gmail.com
In the title molecule, C26H25Br3N2, a dihedral angle of 6.15 (10)° is present between the carbazole and benzene ring systems with an E conformation about the C=C bond [1.335 (4) Å]. The butyl group is almost perpendicular to the carbazole plane [C—N—C—C torsion angle = −98.7 (3)°]. In the crystal, supramolecular double chains along [-7,18,-16] are formed via C—H⋯Br and π–π interactions [centroid(carbazole five-membered ring)⋯centroid(carbazole six-membered ring) distance = 3.6333 (13) Å].
Related literature
For the use of carbazole derivatives in organic light-emitting diodes and photovoltaic devices, see: Thomas et al. (2001, 2004); Wu et al. (2005); Lee et al. (2012); Ooyama et al. (2011). For related structures, see: Pawluć et al. (2011); Zhang & Zhang (2011); Ramathilagam et al. (2011).
Experimental
Crystal data
|
Refinement
|
Data collection: CrysAlis PRO (Agilent, 2010); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536812011336/gg2078sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812011336/gg2078Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812011336/gg2078Isup3.cml
A mixture of 2,3,6,7-tetrabromo-9-butyl-9H-carbazole (0.25 g, 0.47 mmol), styrene (0.29 g, 1.96 mmol), tetrabutylammonium bromide (0.32 g, 0.98 mmol), sodium acetate (1.6 g, 19.6 mmol), Pd(OAc)2 (4 mg) and dimethylformamide (5 ml) was heated at 383 K for 48 h. Subsequently, it was cooled, then poured into water and extracted using ethyl acetate. On removal of solvent, a residue was obtained which on purification by
on silica gel gave an orange crystalline solid. Yield: 0.12 g, 42%. M.pt: 414 K. Crystals were grown from a solution of the title compound dissolved in dichloromethane/hexanes mixture (1:9 v/v).1H NMR (500 MHz, CDCl3) δ: 8.20 (s, 1 H), 8.17 (s, 1 H), 7.63 (s, 1H), 7.58 (s, 1 H), 7.51 (d, J = 9.0 Hz, 2 H), 7.43 (d, J = 16 Hz, 1 H), 7.05 (d, J = 16 Hz, 1 H), 6.74 (d, J = 9 Hz, 2 H), 4.24 (t, J = 7.5 Hz, 2 H), 3.02 (s, 6 H), 1.86–1.83 (m, 2 H), 1.42–1.37 (m, 2 H), 0.97 (t, J = 7.5 Hz, 3 H); 13C NMR (125 MHz, CDCl3) δ: 150.4, 140.7, 140.5, 136.2, 131.4, 128.1, 127.8, 127.4, 125.4, 124.6, 124.4, 124.0, 122.7, 121.6, 121.4, 115.0, 114.0, 113.5, 112.5, 112.4, 105.8, 100.0, 43.2, 40.5, 30.9, 20.6, 13.9.
Carbon-bound H-atoms were placed in calculated positions [C—H = 0.95 to 0.99 Å, Uiso(H) = 1.2 to 1.5Ueq(C)] and were included in the
in the riding model approximation. The maximum and minimum residual electron density peaks of 1.18 and 0.81 e Å-3, respectively, were located 0.86 Å and 0.44 Å from the H2 and Br1 atoms, respectively.Polysubstituted carbazole derivatives have been widely explored as functional materials for applications in organic light-emitting diodes (Thomas et al., 2001; Thomas et al., 2004; Wu et al., 2005) and photovoltaic devices (Lee et al., 2012; Ooyama et al., 2011) due to their charge transporting and amorphous properties. Though the 3,6,9-trisubstituted (Thomas et al., 2001; Thomas et al., 2004) and 2,7,9-trisubstituted carbazole (Wu et al., 2005; Lee et al., 2012) compounds have been well documented in the literature, 2,3,6,7,9-pentasubstituted carbazole derivatives are relatively rare. Herein, the synthesis and
determination of the title compound, (I), are described. Several related structures are known (Pawluć et al., 2011; Zhang & Zhang, 2011; Ramathilagam et al., 2011).In (I), the carbazole fused-ring system is planar with the r.m.s. deviation of the 13 fitted non-hydrogen atoms = 0.006 Å; the Br1, Br2 and Br3 atoms lie 0.058 (1), 0.062 (1) and 0.043 (1) Å out of this plane, respectively. The least-squares plane through the carbazole residue forms a dihedral angle of 6.15 (10)° with the benzene ring, indicating a small twist between the terminal ring systems. This twist is manifested in the value of the C15—C14—C17—C18 torsion angle of -11.2 (4)°. The butyl group is almost perpendicular to the carbazole plane with the C1—N1—C7—C8 torsion angle being -98.7 (3)°. Finally, the conformation about the C17═C18 bond [1.335 (4) Å] is E.
In the crystal packing, molecules are linked into linear supramolecular chains via C—H···Br interactions, Fig. 2 and Table 1. These are connected into double chains along [7 18 16] via π–π interactions occurring between five- and six-membered rings of the carbazole residue [centroid(N1,C1,C6,C11,C16)···centroid(C1–C6)i = 3.6333 (13) Å, angle between rings = 0.50 (12)° for i: 1 - x, 1 - y, -z]. Chains assemble into layers, with no specific interactions between them. In turn, the layers stack along (2 0 2), again without specific interactions between them, Fig. 2.
For the use of carbazole derivatives in organic light-emitting diodes and photovoltaic devices, see: Thomas et al. (2001, 2004); Wu et al. (2005); Lee et al. (2012); Ooyama et al. (2011). For related structures, see: Pawluć et al. (2011); Zhang & Zhang (2011); Ramathilagam et al. (2011).
Data collection: CrysAlis PRO (Agilent, 2010); cell
CrysAlis PRO (Agilent, 2010); data reduction: CrysAlis PRO (Agilent, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).C26H25Br3N2 | Z = 2 |
Mr = 605.21 | F(000) = 600 |
Triclinic, P1 | Dx = 1.730 Mg m−3 |
Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54184 Å |
a = 9.7304 (3) Å | Cell parameters from 7879 reflections |
b = 11.3834 (4) Å | θ = 4.2–76.4° |
c = 11.8197 (4) Å | µ = 6.56 mm−1 |
α = 114.308 (3)° | T = 100 K |
β = 101.957 (3)° | Plate, orange |
γ = 90.127 (3)° | 0.30 × 0.30 × 0.05 mm |
V = 1161.62 (7) Å3 |
Agilent SuperNova Dual diffractometer with an Atlas detector | 4827 independent reflections |
Radiation source: SuperNova (Cu) X-ray Source | 4680 reflections with I > 2σ(I) |
Mirror monochromator | Rint = 0.021 |
Detector resolution: 10.4041 pixels mm-1 | θmax = 76.6°, θmin = 4.2° |
ω scan | h = −12→12 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −14→14 |
Tmin = 0.244, Tmax = 0.735 | l = −14→10 |
10766 measured reflections |
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)] = 0.032 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.092 | H-atom parameters constrained |
S = 1.07 | w = 1/[σ2(Fo2) + (0.0613P)2 + 0.89P] where P = (Fo2 + 2Fc2)/3 |
4827 reflections | (Δ/σ)max = 0.001 |
282 parameters | Δρmax = 1.18 e Å−3 |
0 restraints | Δρmin = −0.81 e Å−3 |
C26H25Br3N2 | γ = 90.127 (3)° |
Mr = 605.21 | V = 1161.62 (7) Å3 |
Triclinic, P1 | Z = 2 |
a = 9.7304 (3) Å | Cu Kα radiation |
b = 11.3834 (4) Å | µ = 6.56 mm−1 |
c = 11.8197 (4) Å | T = 100 K |
α = 114.308 (3)° | 0.30 × 0.30 × 0.05 mm |
β = 101.957 (3)° |
Agilent SuperNova Dual diffractometer with an Atlas detector | 4827 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | 4680 reflections with I > 2σ(I) |
Tmin = 0.244, Tmax = 0.735 | Rint = 0.021 |
10766 measured reflections |
R[F2 > 2σ(F2)] = 0.032 | 0 restraints |
wR(F2) = 0.092 | H-atom parameters constrained |
S = 1.07 | Δρmax = 1.18 e Å−3 |
4827 reflections | Δρmin = −0.81 e Å−3 |
282 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 | ||
Br1 | 0.29708 (3) | 0.83996 (3) | 0.02986 (2) | 0.02733 (9) | |
Br2 | 0.56802 (3) | 0.78783 (3) | −0.11524 (2) | 0.02739 (9) | |
Br3 | 1.11706 (3) | 0.35337 (3) | 0.20455 (3) | 0.02790 (9) | |
N1 | 0.5643 (2) | 0.5740 (2) | 0.27349 (19) | 0.0222 (4) | |
N2 | 1.1308 (3) | 0.0298 (3) | 0.7703 (2) | 0.0333 (5) | |
C1 | 0.5457 (2) | 0.6291 (2) | 0.1869 (2) | 0.0209 (4) | |
C2 | 0.4366 (3) | 0.6979 (2) | 0.1578 (2) | 0.0228 (5) | |
H2 | 0.3598 | 0.7132 | 0.1986 | 0.027* | |
C3 | 0.4443 (3) | 0.7433 (2) | 0.0664 (2) | 0.0226 (5) | |
C4 | 0.5569 (3) | 0.7208 (2) | 0.0055 (2) | 0.0227 (5) | |
C5 | 0.6653 (3) | 0.6523 (2) | 0.0351 (2) | 0.0232 (5) | |
H5 | 0.7418 | 0.6373 | −0.0061 | 0.028* | |
C6 | 0.6601 (2) | 0.6056 (2) | 0.1262 (2) | 0.0205 (4) | |
C7 | 0.4735 (2) | 0.5794 (2) | 0.3587 (2) | 0.0236 (5) | |
H7A | 0.4651 | 0.4940 | 0.3615 | 0.028* | |
H7B | 0.3780 | 0.5967 | 0.3240 | 0.028* | |
C8 | 0.5283 (3) | 0.6836 (2) | 0.4944 (2) | 0.0263 (5) | |
H8A | 0.4684 | 0.6752 | 0.5494 | 0.032* | |
H8B | 0.6253 | 0.6681 | 0.5274 | 0.032* | |
C9 | 0.5301 (3) | 0.8209 (3) | 0.5043 (2) | 0.0295 (5) | |
H9A | 0.4321 | 0.8398 | 0.4793 | 0.035* | |
H9B | 0.5833 | 0.8280 | 0.4441 | 0.035* | |
C10 | 0.5972 (3) | 0.9205 (3) | 0.6384 (3) | 0.0357 (6) | |
H10A | 0.5967 | 1.0074 | 0.6403 | 0.054* | |
H10B | 0.6947 | 0.9029 | 0.6632 | 0.054* | |
H10C | 0.5434 | 0.9155 | 0.6980 | 0.054* | |
C11 | 0.7525 (3) | 0.5336 (2) | 0.1799 (2) | 0.0213 (4) | |
C12 | 0.8799 (3) | 0.4835 (2) | 0.1613 (2) | 0.0223 (5) | |
H12 | 0.9246 | 0.4940 | 0.1014 | 0.027* | |
C13 | 0.9406 (2) | 0.4177 (2) | 0.2322 (2) | 0.0217 (4) | |
C14 | 0.8789 (2) | 0.3989 (2) | 0.3234 (2) | 0.0207 (4) | |
C15 | 0.7510 (3) | 0.4504 (2) | 0.3406 (2) | 0.0216 (4) | |
H15 | 0.7059 | 0.4402 | 0.4004 | 0.026* | |
C16 | 0.6895 (2) | 0.5168 (2) | 0.2704 (2) | 0.0207 (4) | |
C17 | 0.9466 (2) | 0.3259 (2) | 0.3949 (2) | 0.0211 (4) | |
H17 | 1.0239 | 0.2799 | 0.3683 | 0.025* | |
C18 | 0.9070 (3) | 0.3201 (2) | 0.4942 (2) | 0.0238 (5) | |
H18 | 0.8316 | 0.3687 | 0.5218 | 0.029* | |
C19 | 0.9685 (3) | 0.2460 (2) | 0.5642 (2) | 0.0222 (5) | |
C20 | 0.9072 (3) | 0.2399 (3) | 0.6593 (2) | 0.0258 (5) | |
H20 | 0.8267 | 0.2851 | 0.6769 | 0.031* | |
C21 | 0.9600 (3) | 0.1702 (3) | 0.7288 (3) | 0.0274 (5) | |
H21 | 0.9152 | 0.1683 | 0.7923 | 0.033* | |
C22 | 1.0787 (3) | 0.1029 (2) | 0.7058 (2) | 0.0245 (5) | |
C23 | 1.1426 (3) | 0.1108 (2) | 0.6119 (2) | 0.0253 (5) | |
H23 | 1.2248 | 0.0679 | 0.5958 | 0.030* | |
C24 | 1.0881 (3) | 0.1797 (2) | 0.5433 (2) | 0.0243 (5) | |
H24 | 1.1331 | 0.1822 | 0.4801 | 0.029* | |
C25 | 1.2647 (3) | −0.0235 (3) | 0.7574 (3) | 0.0300 (5) | |
H25A | 1.3375 | 0.0461 | 0.7772 | 0.045* | |
H25B | 1.2562 | −0.0885 | 0.6698 | 0.045* | |
H25C | 1.2909 | −0.0641 | 0.8166 | 0.045* | |
C26 | 1.0606 (3) | 0.0186 (3) | 0.8627 (3) | 0.0328 (6) | |
H26A | 0.9602 | −0.0093 | 0.8233 | 0.049* | |
H26B | 1.0708 | 0.1029 | 0.9360 | 0.049* | |
H26C | 1.1033 | −0.0453 | 0.8912 | 0.049* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.02941 (16) | 0.02848 (15) | 0.02854 (15) | 0.00817 (11) | 0.00398 (11) | 0.01757 (11) |
Br2 | 0.03297 (16) | 0.03048 (15) | 0.02791 (15) | 0.00781 (11) | 0.00784 (11) | 0.02082 (12) |
Br3 | 0.02538 (15) | 0.03522 (16) | 0.03272 (16) | 0.01107 (11) | 0.01128 (11) | 0.02151 (12) |
N1 | 0.0211 (9) | 0.0276 (10) | 0.0239 (9) | 0.0051 (8) | 0.0045 (8) | 0.0172 (8) |
N2 | 0.0314 (12) | 0.0441 (13) | 0.0403 (13) | 0.0144 (10) | 0.0105 (10) | 0.0322 (11) |
C1 | 0.0224 (11) | 0.0212 (10) | 0.0206 (10) | 0.0004 (9) | 0.0019 (8) | 0.0117 (9) |
C2 | 0.0244 (11) | 0.0240 (11) | 0.0226 (11) | 0.0030 (9) | 0.0040 (9) | 0.0130 (9) |
C3 | 0.0235 (11) | 0.0209 (10) | 0.0229 (11) | 0.0036 (9) | 0.0010 (9) | 0.0109 (9) |
C4 | 0.0295 (12) | 0.0206 (10) | 0.0194 (10) | 0.0024 (9) | 0.0017 (9) | 0.0117 (9) |
C5 | 0.0274 (12) | 0.0224 (11) | 0.0224 (11) | 0.0022 (9) | 0.0060 (9) | 0.0119 (9) |
C6 | 0.0229 (11) | 0.0194 (10) | 0.0196 (10) | 0.0016 (8) | 0.0024 (8) | 0.0097 (9) |
C7 | 0.0200 (11) | 0.0291 (12) | 0.0287 (12) | 0.0031 (9) | 0.0068 (9) | 0.0184 (10) |
C8 | 0.0274 (12) | 0.0322 (13) | 0.0270 (12) | 0.0070 (10) | 0.0095 (9) | 0.0184 (10) |
C9 | 0.0344 (13) | 0.0315 (13) | 0.0281 (12) | 0.0033 (10) | 0.0084 (10) | 0.0172 (11) |
C10 | 0.0428 (16) | 0.0347 (14) | 0.0303 (13) | 0.0040 (12) | 0.0104 (12) | 0.0133 (11) |
C11 | 0.0242 (11) | 0.0199 (10) | 0.0212 (11) | 0.0006 (9) | 0.0022 (9) | 0.0116 (9) |
C12 | 0.0254 (12) | 0.0231 (11) | 0.0211 (11) | 0.0018 (9) | 0.0051 (9) | 0.0120 (9) |
C13 | 0.0193 (11) | 0.0225 (10) | 0.0238 (11) | 0.0021 (8) | 0.0035 (9) | 0.0109 (9) |
C14 | 0.0198 (11) | 0.0218 (11) | 0.0216 (11) | 0.0014 (8) | 0.0024 (8) | 0.0112 (9) |
C15 | 0.0238 (11) | 0.0227 (11) | 0.0230 (11) | 0.0029 (9) | 0.0037 (9) | 0.0150 (9) |
C16 | 0.0203 (11) | 0.0217 (10) | 0.0215 (11) | 0.0023 (8) | 0.0020 (8) | 0.0118 (9) |
C17 | 0.0206 (10) | 0.0193 (10) | 0.0239 (11) | 0.0013 (8) | 0.0018 (8) | 0.0112 (9) |
C18 | 0.0230 (11) | 0.0240 (11) | 0.0262 (11) | 0.0056 (9) | 0.0028 (9) | 0.0137 (9) |
C19 | 0.0214 (11) | 0.0235 (11) | 0.0240 (11) | 0.0017 (9) | 0.0023 (9) | 0.0136 (9) |
C20 | 0.0220 (11) | 0.0318 (12) | 0.0301 (12) | 0.0086 (9) | 0.0080 (9) | 0.0183 (10) |
C21 | 0.0257 (12) | 0.0344 (13) | 0.0292 (12) | 0.0037 (10) | 0.0069 (10) | 0.0200 (11) |
C22 | 0.0234 (11) | 0.0261 (11) | 0.0285 (12) | 0.0036 (9) | 0.0021 (9) | 0.0177 (10) |
C23 | 0.0228 (11) | 0.0272 (12) | 0.0303 (12) | 0.0061 (9) | 0.0061 (9) | 0.0164 (10) |
C24 | 0.0238 (11) | 0.0262 (12) | 0.0274 (12) | 0.0045 (9) | 0.0055 (9) | 0.0160 (10) |
C25 | 0.0283 (13) | 0.0314 (13) | 0.0345 (13) | 0.0084 (10) | 0.0028 (10) | 0.0200 (11) |
C26 | 0.0347 (14) | 0.0421 (15) | 0.0350 (14) | 0.0110 (12) | 0.0093 (11) | 0.0286 (12) |
Br1—C3 | 1.895 (2) | C11—C12 | 1.386 (3) |
Br2—C4 | 1.895 (2) | C11—C16 | 1.413 (3) |
Br3—C13 | 1.906 (2) | C12—C13 | 1.388 (3) |
N1—C16 | 1.382 (3) | C12—H12 | 0.9500 |
N1—C1 | 1.388 (3) | C13—C14 | 1.423 (3) |
N1—C7 | 1.455 (3) | C14—C15 | 1.394 (3) |
N2—C22 | 1.378 (3) | C14—C17 | 1.479 (3) |
N2—C26 | 1.447 (3) | C15—C16 | 1.389 (3) |
N2—C25 | 1.448 (3) | C15—H15 | 0.9500 |
C1—C2 | 1.390 (3) | C17—C18 | 1.335 (4) |
C1—C6 | 1.415 (3) | C17—H17 | 0.9500 |
C2—C3 | 1.390 (3) | C18—C19 | 1.458 (3) |
C2—H2 | 0.9500 | C18—H18 | 0.9500 |
C3—C4 | 1.401 (4) | C19—C24 | 1.398 (3) |
C4—C5 | 1.385 (3) | C19—C20 | 1.401 (3) |
C5—C6 | 1.393 (3) | C20—C21 | 1.390 (4) |
C5—H5 | 0.9500 | C20—H20 | 0.9500 |
C6—C11 | 1.442 (3) | C21—C22 | 1.399 (4) |
C7—C8 | 1.530 (4) | C21—H21 | 0.9500 |
C7—H7A | 0.9900 | C22—C23 | 1.412 (3) |
C7—H7B | 0.9900 | C23—C24 | 1.379 (3) |
C8—C9 | 1.518 (4) | C23—H23 | 0.9500 |
C8—H8A | 0.9900 | C24—H24 | 0.9500 |
C8—H8B | 0.9900 | C25—H25A | 0.9800 |
C9—C10 | 1.520 (4) | C25—H25B | 0.9800 |
C9—H9A | 0.9900 | C25—H25C | 0.9800 |
C9—H9B | 0.9900 | C26—H26A | 0.9800 |
C10—H10A | 0.9800 | C26—H26B | 0.9800 |
C10—H10B | 0.9800 | C26—H26C | 0.9800 |
C10—H10C | 0.9800 | ||
C16—N1—C1 | 108.3 (2) | C11—C12—C13 | 118.5 (2) |
C16—N1—C7 | 124.7 (2) | C11—C12—H12 | 120.7 |
C1—N1—C7 | 126.9 (2) | C13—C12—H12 | 120.7 |
C22—N2—C26 | 120.0 (2) | C12—C13—C14 | 123.4 (2) |
C22—N2—C25 | 120.1 (2) | C12—C13—Br3 | 116.64 (18) |
C26—N2—C25 | 119.5 (2) | C14—C13—Br3 | 119.95 (18) |
C2—C1—N1 | 129.2 (2) | C15—C14—C13 | 117.0 (2) |
C2—C1—C6 | 121.6 (2) | C15—C14—C17 | 121.7 (2) |
N1—C1—C6 | 109.1 (2) | C13—C14—C17 | 121.3 (2) |
C1—C2—C3 | 117.4 (2) | C14—C15—C16 | 120.1 (2) |
C1—C2—H2 | 121.3 | C14—C15—H15 | 119.9 |
C3—C2—H2 | 121.3 | C16—C15—H15 | 119.9 |
C2—C3—C4 | 121.7 (2) | N1—C16—C15 | 128.7 (2) |
C2—C3—Br1 | 117.04 (19) | N1—C16—C11 | 109.5 (2) |
C4—C3—Br1 | 121.27 (18) | C15—C16—C11 | 121.8 (2) |
C5—C4—C3 | 120.7 (2) | C18—C17—C14 | 124.7 (2) |
C5—C4—Br2 | 118.33 (19) | C18—C17—H17 | 117.7 |
C3—C4—Br2 | 120.98 (18) | C14—C17—H17 | 117.7 |
C4—C5—C6 | 118.8 (2) | C17—C18—C19 | 126.1 (2) |
C4—C5—H5 | 120.6 | C17—C18—H18 | 117.0 |
C6—C5—H5 | 120.6 | C19—C18—H18 | 117.0 |
C5—C6—C1 | 119.8 (2) | C24—C19—C20 | 116.7 (2) |
C5—C6—C11 | 133.5 (2) | C24—C19—C18 | 123.8 (2) |
C1—C6—C11 | 106.6 (2) | C20—C19—C18 | 119.5 (2) |
N1—C7—C8 | 112.9 (2) | C21—C20—C19 | 122.3 (2) |
N1—C7—H7A | 109.0 | C21—C20—H20 | 118.8 |
C8—C7—H7A | 109.0 | C19—C20—H20 | 118.8 |
N1—C7—H7B | 109.0 | C20—C21—C22 | 120.4 (2) |
C8—C7—H7B | 109.0 | C20—C21—H21 | 119.8 |
H7A—C7—H7B | 107.8 | C22—C21—H21 | 119.8 |
C9—C8—C7 | 114.0 (2) | N2—C22—C21 | 121.7 (2) |
C9—C8—H8A | 108.8 | N2—C22—C23 | 120.8 (2) |
C7—C8—H8A | 108.8 | C21—C22—C23 | 117.5 (2) |
C9—C8—H8B | 108.8 | C24—C23—C22 | 121.3 (2) |
C7—C8—H8B | 108.8 | C24—C23—H23 | 119.4 |
H8A—C8—H8B | 107.7 | C22—C23—H23 | 119.4 |
C8—C9—C10 | 112.2 (2) | C23—C24—C19 | 121.7 (2) |
C8—C9—H9A | 109.2 | C23—C24—H24 | 119.1 |
C10—C9—H9A | 109.2 | C19—C24—H24 | 119.1 |
C8—C9—H9B | 109.2 | N2—C25—H25A | 109.5 |
C10—C9—H9B | 109.2 | N2—C25—H25B | 109.5 |
H9A—C9—H9B | 107.9 | H25A—C25—H25B | 109.5 |
C9—C10—H10A | 109.5 | N2—C25—H25C | 109.5 |
C9—C10—H10B | 109.5 | H25A—C25—H25C | 109.5 |
H10A—C10—H10B | 109.5 | H25B—C25—H25C | 109.5 |
C9—C10—H10C | 109.5 | N2—C26—H26A | 109.5 |
H10A—C10—H10C | 109.5 | N2—C26—H26B | 109.5 |
H10B—C10—H10C | 109.5 | H26A—C26—H26B | 109.5 |
C12—C11—C16 | 119.2 (2) | N2—C26—H26C | 109.5 |
C12—C11—C6 | 134.4 (2) | H26A—C26—H26C | 109.5 |
C16—C11—C6 | 106.4 (2) | H26B—C26—H26C | 109.5 |
C16—N1—C1—C2 | −179.3 (2) | C12—C13—C14—C17 | 178.9 (2) |
C7—N1—C1—C2 | −2.2 (4) | Br3—C13—C14—C17 | −2.1 (3) |
C16—N1—C1—C6 | 0.7 (3) | C13—C14—C15—C16 | −0.1 (3) |
C7—N1—C1—C6 | 177.8 (2) | C17—C14—C15—C16 | −179.1 (2) |
N1—C1—C2—C3 | 179.8 (2) | C1—N1—C16—C15 | 180.0 (2) |
C6—C1—C2—C3 | −0.2 (4) | C7—N1—C16—C15 | 2.7 (4) |
C1—C2—C3—C4 | 0.2 (4) | C1—N1—C16—C11 | −0.6 (3) |
C1—C2—C3—Br1 | −178.73 (17) | C7—N1—C16—C11 | −177.9 (2) |
C2—C3—C4—C5 | −0.2 (4) | C14—C15—C16—N1 | 179.8 (2) |
Br1—C3—C4—C5 | 178.67 (18) | C14—C15—C16—C11 | 0.4 (4) |
C2—C3—C4—Br2 | −178.20 (19) | C12—C11—C16—N1 | 180.0 (2) |
Br1—C3—C4—Br2 | 0.6 (3) | C6—C11—C16—N1 | 0.4 (3) |
C3—C4—C5—C6 | 0.2 (4) | C12—C11—C16—C15 | −0.6 (3) |
Br2—C4—C5—C6 | 178.27 (18) | C6—C11—C16—C15 | 179.8 (2) |
C4—C5—C6—C1 | −0.2 (4) | C15—C14—C17—C18 | −11.2 (4) |
C4—C5—C6—C11 | −179.3 (2) | C13—C14—C17—C18 | 169.8 (2) |
C2—C1—C6—C5 | 0.2 (4) | C14—C17—C18—C19 | 178.0 (2) |
N1—C1—C6—C5 | −179.8 (2) | C17—C18—C19—C24 | 6.3 (4) |
C2—C1—C6—C11 | 179.5 (2) | C17—C18—C19—C20 | −174.2 (2) |
N1—C1—C6—C11 | −0.4 (3) | C24—C19—C20—C21 | −1.0 (4) |
C16—N1—C7—C8 | 78.0 (3) | C18—C19—C20—C21 | 179.5 (2) |
C1—N1—C7—C8 | −98.7 (3) | C19—C20—C21—C22 | 0.2 (4) |
N1—C7—C8—C9 | 65.2 (3) | C26—N2—C22—C21 | 1.4 (4) |
C7—C8—C9—C10 | −175.0 (2) | C25—N2—C22—C21 | −171.3 (2) |
C5—C6—C11—C12 | −0.2 (5) | C26—N2—C22—C23 | −177.6 (3) |
C1—C6—C11—C12 | −179.5 (3) | C25—N2—C22—C23 | 9.7 (4) |
C5—C6—C11—C16 | 179.3 (3) | C20—C21—C22—N2 | −178.0 (3) |
C1—C6—C11—C16 | 0.0 (3) | C20—C21—C22—C23 | 1.1 (4) |
C16—C11—C12—C13 | 0.4 (3) | N2—C22—C23—C24 | 177.5 (3) |
C6—C11—C12—C13 | 179.8 (2) | C21—C22—C23—C24 | −1.6 (4) |
C11—C12—C13—C14 | 0.0 (4) | C22—C23—C24—C19 | 0.8 (4) |
C11—C12—C13—Br3 | −179.05 (17) | C20—C19—C24—C23 | 0.6 (4) |
C12—C13—C14—C15 | −0.2 (4) | C18—C19—C24—C23 | 180.0 (2) |
Br3—C13—C14—C15 | 178.85 (17) |
D—H···A | D—H | H···A | D···A | D—H···A |
C26—H26C···Br1i | 0.98 | 2.91 | 3.844 (3) | 161 |
Symmetry code: (i) x+1, y−1, z+1. |
Experimental details
Crystal data | |
Chemical formula | C26H25Br3N2 |
Mr | 605.21 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 100 |
a, b, c (Å) | 9.7304 (3), 11.3834 (4), 11.8197 (4) |
α, β, γ (°) | 114.308 (3), 101.957 (3), 90.127 (3) |
V (Å3) | 1161.62 (7) |
Z | 2 |
Radiation type | Cu Kα |
µ (mm−1) | 6.56 |
Crystal size (mm) | 0.30 × 0.30 × 0.05 |
Data collection | |
Diffractometer | Agilent SuperNova Dual diffractometer with an Atlas detector |
Absorption correction | Multi-scan (CrysAlis PRO; Agilent, 2010) |
Tmin, Tmax | 0.244, 0.735 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 10766, 4827, 4680 |
Rint | 0.021 |
(sin θ/λ)max (Å−1) | 0.631 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.032, 0.092, 1.07 |
No. of reflections | 4827 |
No. of parameters | 282 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.18, −0.81 |
Computer programs: CrysAlis PRO (Agilent, 2010), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
C26—H26C···Br1i | 0.98 | 2.91 | 3.844 (3) | 161 |
Symmetry code: (i) x+1, y−1, z+1. |
Footnotes
‡Additional correspondence author: krjt8fcy@iitr.ernet.in.
Acknowledgements
KRJT thanks the Council of Scientific and Industrial Research (CSIR), New Delhi, for financial support [grant No. 01 (2111)/07/EMR-II)]. The authors also thank the Ministry of Higher Education (Malaysia) for funding structural studies through the High-Impact Research scheme (grant No. UM.C/HIR/MOHE/SC/12).
References
Agilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, Oxfordshire, England. Google Scholar
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Lee, W., Cho, N., Kwon, J., Ko, J. & Hong, J.-I. (2012). Chem. Asian J. 7, 343–350. Web of Science CrossRef CAS PubMed Google Scholar
Ooyama, Y., Nagno, T., Inou, S., Imae, I., Komaguchi, K., Ohshita, J. & Harima, Y. (2011). Chem. Eur. J. 17, 14837–14843. Web of Science CrossRef CAS PubMed Google Scholar
Pawluć, P., Franczyk, A., Walkowiak, J., Hreczycho, G., Kubicki, M. & Marciniec, B. (2011). Org. Lett. 13, 1976–1979. Web of Science PubMed Google Scholar
Ramathilagam, C., Venkatesan, N., Rajakumar, P., Umarani, P. R. & Manivannan, V. (2011). Acta Cryst. E67, o2796. Web of Science CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Thomas, K. R. J., Lin, J. T., Tao, Y.-T. & Chuan, C.-H. (2004). Chem. Mater. 16, 5437–5444. CAS Google Scholar
Thomas, K. R. J., Lin, J. T., Tao, Y.-T. & Ko, C.-W. (2001). J. Am. Chem. Soc. 123, 9404–9411. Web of Science CSD CrossRef PubMed CAS Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
Wu, F.-I., Shih, P.-I., Yuan, M.-C., Dixit, A. K., Shu, C.-F., Chung, Z.-M. & Diau, E. W.-G. (2005). J. Mater. Chem. 15, 4753–4760. Web of Science CrossRef CAS Google Scholar
Zhang, J.-Y. & Zhang, W.-Y. (2011). Acta Cryst. E67, o3307. Web of Science CSD CrossRef IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Polysubstituted carbazole derivatives have been widely explored as functional materials for applications in organic light-emitting diodes (Thomas et al., 2001; Thomas et al., 2004; Wu et al., 2005) and photovoltaic devices (Lee et al., 2012; Ooyama et al., 2011) due to their charge transporting and amorphous properties. Though the 3,6,9-trisubstituted (Thomas et al., 2001; Thomas et al., 2004) and 2,7,9-trisubstituted carbazole (Wu et al., 2005; Lee et al., 2012) compounds have been well documented in the literature, 2,3,6,7,9-pentasubstituted carbazole derivatives are relatively rare. Herein, the synthesis and crystal structure determination of the title compound, (I), are described. Several related structures are known (Pawluć et al., 2011; Zhang & Zhang, 2011; Ramathilagam et al., 2011).
In (I), the carbazole fused-ring system is planar with the r.m.s. deviation of the 13 fitted non-hydrogen atoms = 0.006 Å; the Br1, Br2 and Br3 atoms lie 0.058 (1), 0.062 (1) and 0.043 (1) Å out of this plane, respectively. The least-squares plane through the carbazole residue forms a dihedral angle of 6.15 (10)° with the benzene ring, indicating a small twist between the terminal ring systems. This twist is manifested in the value of the C15—C14—C17—C18 torsion angle of -11.2 (4)°. The butyl group is almost perpendicular to the carbazole plane with the C1—N1—C7—C8 torsion angle being -98.7 (3)°. Finally, the conformation about the C17═C18 bond [1.335 (4) Å] is E.
In the crystal packing, molecules are linked into linear supramolecular chains via C—H···Br interactions, Fig. 2 and Table 1. These are connected into double chains along [7 18 16] via π–π interactions occurring between five- and six-membered rings of the carbazole residue [centroid(N1,C1,C6,C11,C16)···centroid(C1–C6)i = 3.6333 (13) Å, angle between rings = 0.50 (12)° for symmetry operation i: 1 - x, 1 - y, -z]. Chains assemble into layers, with no specific interactions between them. In turn, the layers stack along (2 0 2), again without specific interactions between them, Fig. 2.