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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jan 15;67(Pt 2):o417. doi: 10.1107/S160053681100119X

4-(1-Ethyl-1H-1,3-benzimidazol-2-yl)-N,N-diphenyl­aniline monohydrate

Tao Wu a, Kai Wang a, Peng Jiang a, Hong-Jun Zhu a,*
PMCID: PMC3051646  PMID: 21523087

Abstract

In the title compound, C27H23N3O·H2O, the benzimidazole ring system has an r.m.s. deviation of 0.0071 Å and makes dihedral angles of 34.51 (2), 55.22 (3) and 41.05 (5)° with the central and N-bonded phenyl rings, respectively. In the crystal, the water mol­ecular is connected to the organic mol­ecule by inter­molecular O—H⋯N hydrogen bonds. Weak inter­molecular C—H⋯O hydrogen bonds also occur.

Related literature

For the synthetic procedure, see: Vinodkumar et al. (2008). For bond-length data, see: Allen et al. (1987). For background to the use of the title compound as an inter­mediate in the preparation of OLED materials, see: Kakimoto et al. (2008). graphic file with name e-67-0o417-scheme1.jpg

Experimental

Crystal data

  • C27H23N3·H2O

  • M r = 407.50

  • Monoclinic, Inline graphic

  • a = 12.278 (3) Å

  • b = 9.2690 (19) Å

  • c = 19.468 (4) Å

  • β = 97.81 (3)°

  • V = 2195.0 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 K

  • 0.30 × 0.20 × 0.10 mm

Data collection

  • Enraf–Nonius CAD-4 diffractometer

  • Absorption correction: ψ scan (North et al., 1968) T min = 0.978, T max = 0.992

  • 4223 measured reflections

  • 4024 independent reflections

  • 2487 reflections with I > 2σ(I)

  • R int = 0.025

  • 3 standard reflections every 200 reflections intensity decay: 1%

Refinement

  • R[F 2 > 2σ(F 2)] = 0.057

  • wR(F 2) = 0.169

  • S = 1.01

  • 4024 reflections

  • 281 parameters

  • H-atom parameters constrained

  • Δρmax = 0.18 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: CAD-4 Software (Enraf–Nonius, 1985); cell refinement: CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo, 1995); 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/S160053681100119X/bq2268sup1.cif

e-67-0o417-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681100119X/bq2268Isup2.hkl

e-67-0o417-Isup2.hkl (197.2KB, 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
OW—HWB⋯N2 0.85 2.50 2.903 (3) 110
OW—HWA⋯N2 0.85 2.49 2.903 (3) 111
C24—H24A⋯OWi 0.93 2.43 3.352 (4) 173

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the Center of Testing and Analysis, Nanjing University, for support.

supplementary crystallographic information

Comment

The title compound, (I), is a kind of important organic intermediate which can be used for many fields such as OLED materials. (Kakimoto et al., 2008). We herein report its crystal structure.

In the molecule of (I), (Fig.1), the bond lengths (Allen et al., 1987) and angles are within normal ranges. The benzimidazole ring (A) is obviously almost coplanar with an r.m.s. deviation of 0.0071 °. The dihedral angles between A and the rest three phenyl rings B (C13-C18), C (C7-C12) and D (C1-C6) are 34.51 (2) ° 55.22 (3) ° and 41.05 (5) °, respectively. The H2O molecule stems from the solvent ethanol, and the water molecular is connected with the target molecular by intermolecular C—H···O and O—H···N hydrogen bonds (Table 1), which seems to be very effective in the stabilization of the crystal structure.

Experimental

The title compound, (I) was synthesized according to the literature (Vinodkumar et al., 2008) The crystals were obtained by dissolving (I) (0.52 g, 1.28 mmol) in 25 ml ethanol and evaporating the solvent slowly at room temperature for about 7 d.

Refinement

H atoms bonded to N and O atoms were located in a difference map and refined with distance restraints of O—H = 0.85 (2) and N—H = 0.90 (2) Å, and with Uiso(H) = 1.2Ueq(N,O). Other H atoms were positioned geometrically and refined using a riding model, with C—H = 0.93 - 0.97 (2) Å, Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I), with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

A packing diagram of (I). Hydrogen bonds are shown as dashed lines.

Crystal data

C27H23N3·H2O F(000) = 864
Mr = 407.50 Dx = 1.233 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 25 reflections
a = 12.278 (3) Å θ = 10–14°
b = 9.2690 (19) Å µ = 0.08 mm1
c = 19.468 (4) Å T = 293 K
β = 97.81 (3)° Block, colorless
V = 2195.0 (8) Å3 0.30 × 0.20 × 0.10 mm
Z = 4

Data collection

Enraf–Nonius CAD-4 diffractometer 2487 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.025
graphite θmax = 25.4°, θmin = 1.7°
ω/2θ scans h = 0→14
Absorption correction: ψ scan (North et al., 1968) k = 0→11
Tmin = 0.978, Tmax = 0.992 l = −23→23
4223 measured reflections 3 standard reflections every 200 reflections
4024 independent reflections intensity decay: 1%

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)] = 0.057 H-atom parameters constrained
wR(F2) = 0.169 w = 1/[σ2(Fo2) + (0.090P)2] where P = (Fo2 + 2Fc2)/3
S = 1.01 (Δ/σ)max < 0.001
4024 reflections Δρmax = 0.18 e Å3
281 parameters Δρmin = −0.26 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: 0.0093 (17)

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
N1 0.12417 (17) 0.8084 (2) −0.08205 (12) 0.0535 (6)
C1 0.0167 (2) 1.0299 (3) −0.09280 (14) 0.0502 (7)
H1A −0.0468 0.9764 −0.0906 0.060*
N2 0.53509 (16) 0.6320 (2) 0.14215 (10) 0.0457 (5)
C2 0.0102 (2) 1.1782 (3) −0.10031 (16) 0.0599 (8)
H2B −0.0578 1.2238 −0.1038 0.072*
N3 0.47737 (16) 0.4037 (2) 0.12179 (11) 0.0435 (5)
C3 0.1033 (3) 1.2582 (3) −0.10260 (16) 0.0622 (8)
H3A 0.0986 1.3580 −0.1072 0.075*
C4 0.2031 (2) 1.1914 (3) −0.09818 (15) 0.0567 (7)
H4A 0.2664 1.2461 −0.0993 0.068*
C5 0.2108 (2) 1.0429 (3) −0.09211 (14) 0.0522 (7)
H5A 0.2787 0.9977 −0.0905 0.063*
C6 0.1169 (2) 0.9614 (3) −0.08850 (13) 0.0442 (6)
C7 0.03574 (19) 0.7225 (3) −0.11420 (13) 0.0419 (6)
C8 −0.0220 (2) 0.6349 (3) −0.07465 (15) 0.0514 (7)
H8A −0.0017 0.6299 −0.0269 0.062*
C9 −0.1095 (2) 0.5549 (3) −0.10554 (18) 0.0625 (8)
H9A −0.1477 0.4955 −0.0786 0.075*
C10 −0.1405 (3) 0.5620 (3) −0.1750 (2) 0.0737 (10)
H10A −0.2004 0.5088 −0.1956 0.088*
C11 −0.0834 (3) 0.6476 (4) −0.21467 (17) 0.0733 (9)
H11A −0.1042 0.6516 −0.2624 0.088*
C12 0.0048 (2) 0.7282 (3) −0.18469 (14) 0.0609 (8)
H12A 0.0433 0.7861 −0.2121 0.073*
C13 0.20766 (19) 0.7440 (3) −0.03508 (13) 0.0431 (6)
C14 0.2497 (2) 0.8104 (3) 0.02666 (13) 0.0461 (6)
H14A 0.2234 0.9005 0.0375 0.055*
C15 0.3298 (2) 0.7442 (3) 0.07189 (13) 0.0443 (6)
H15A 0.3578 0.7910 0.1128 0.053*
C16 0.37033 (19) 0.6077 (3) 0.05776 (13) 0.0408 (6)
C17 0.32912 (19) 0.5432 (3) −0.00436 (13) 0.0435 (6)
H17A 0.3560 0.4536 −0.0154 0.052*
C18 0.2488 (2) 0.6091 (3) −0.05033 (13) 0.0446 (6)
H18A 0.2220 0.5633 −0.0917 0.053*
C19 0.4598 (2) 0.5481 (3) 0.10699 (13) 0.0419 (6)
C20 0.6054 (2) 0.5389 (3) 0.18193 (13) 0.0457 (6)
C21 0.6991 (2) 0.5681 (3) 0.22815 (14) 0.0560 (7)
H21A 0.7225 0.6625 0.2371 0.067*
C22 0.7562 (3) 0.4543 (4) 0.26021 (16) 0.0706 (9)
H22A 0.8196 0.4716 0.2910 0.085*
C23 0.7204 (3) 0.3122 (3) 0.24720 (16) 0.0681 (9)
H23A 0.7611 0.2374 0.2697 0.082*
C24 0.6278 (2) 0.2793 (3) 0.20264 (15) 0.0587 (8)
H24A 0.6040 0.1847 0.1947 0.070*
C25 0.5710 (2) 0.3962 (3) 0.16973 (13) 0.0443 (6)
C26 0.4069 (2) 0.2785 (3) 0.10055 (15) 0.0556 (7)
H26A 0.3350 0.3125 0.0803 0.067*
H26B 0.3975 0.2221 0.1413 0.067*
C27 0.4534 (3) 0.1826 (3) 0.04887 (17) 0.0717 (9)
H27A 0.4046 0.1029 0.0370 0.108*
H27B 0.5241 0.1471 0.0689 0.108*
H27C 0.4611 0.2371 0.0079 0.108*
OW 0.5578 (2) 0.9300 (3) 0.18768 (15) 0.1158 (10)
HWB 0.5151 0.8673 0.2015 0.139*
HWA 0.5919 0.8888 0.1579 0.139*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0452 (12) 0.0373 (12) 0.0720 (15) −0.0054 (10) −0.0136 (11) 0.0103 (11)
C1 0.0447 (15) 0.0436 (16) 0.0618 (18) −0.0048 (12) 0.0060 (13) −0.0013 (13)
N2 0.0466 (12) 0.0395 (12) 0.0487 (13) 0.0007 (10) −0.0017 (10) 0.0037 (10)
C2 0.0593 (18) 0.0438 (17) 0.076 (2) 0.0047 (14) 0.0084 (15) −0.0064 (14)
N3 0.0456 (12) 0.0314 (11) 0.0524 (13) −0.0009 (9) 0.0030 (10) 0.0064 (9)
C3 0.076 (2) 0.0335 (15) 0.076 (2) −0.0049 (15) 0.0059 (17) −0.0042 (14)
C4 0.0601 (18) 0.0439 (17) 0.0637 (18) −0.0169 (14) −0.0005 (14) 0.0051 (14)
C5 0.0432 (14) 0.0482 (16) 0.0631 (18) −0.0050 (13) −0.0007 (13) 0.0064 (14)
C6 0.0455 (14) 0.0373 (14) 0.0476 (15) −0.0025 (12) −0.0012 (12) 0.0054 (12)
C7 0.0381 (13) 0.0333 (13) 0.0520 (16) −0.0002 (11) −0.0019 (12) 0.0013 (11)
C8 0.0511 (15) 0.0469 (16) 0.0554 (17) −0.0007 (13) 0.0041 (13) 0.0050 (13)
C9 0.0478 (16) 0.0487 (17) 0.090 (2) −0.0096 (14) 0.0067 (16) 0.0052 (16)
C10 0.0583 (19) 0.0508 (19) 0.104 (3) −0.0061 (16) −0.0186 (19) −0.0158 (19)
C11 0.085 (2) 0.071 (2) 0.0557 (19) 0.004 (2) −0.0171 (18) −0.0122 (17)
C12 0.0669 (19) 0.0648 (19) 0.0495 (17) −0.0021 (16) 0.0026 (15) 0.0044 (14)
C13 0.0378 (13) 0.0357 (14) 0.0544 (16) −0.0037 (11) 0.0013 (12) 0.0076 (12)
C14 0.0448 (14) 0.0386 (14) 0.0537 (16) 0.0036 (12) 0.0025 (12) −0.0012 (12)
C15 0.0458 (14) 0.0399 (14) 0.0458 (15) −0.0016 (12) 0.0009 (12) −0.0031 (11)
C16 0.0377 (13) 0.0367 (14) 0.0476 (15) −0.0032 (11) 0.0040 (11) 0.0025 (11)
C17 0.0415 (13) 0.0332 (13) 0.0560 (16) −0.0002 (11) 0.0073 (12) −0.0011 (12)
C18 0.0450 (14) 0.0381 (14) 0.0487 (15) −0.0049 (12) −0.0003 (12) −0.0016 (12)
C19 0.0430 (13) 0.0360 (14) 0.0469 (14) −0.0002 (12) 0.0063 (11) 0.0028 (12)
C20 0.0463 (15) 0.0440 (15) 0.0460 (15) 0.0011 (12) 0.0041 (12) 0.0036 (12)
C21 0.0570 (17) 0.0506 (17) 0.0563 (17) −0.0022 (14) −0.0067 (14) 0.0013 (14)
C22 0.0651 (19) 0.076 (2) 0.064 (2) 0.0051 (18) −0.0142 (16) 0.0095 (17)
C23 0.072 (2) 0.061 (2) 0.067 (2) 0.0176 (17) −0.0079 (17) 0.0206 (16)
C24 0.0676 (19) 0.0433 (16) 0.0645 (19) 0.0062 (14) 0.0067 (16) 0.0122 (14)
C25 0.0469 (14) 0.0404 (14) 0.0458 (15) 0.0033 (12) 0.0072 (12) 0.0076 (12)
C26 0.0544 (16) 0.0392 (15) 0.0715 (19) −0.0095 (13) 0.0032 (14) 0.0105 (14)
C27 0.077 (2) 0.0437 (17) 0.091 (2) −0.0017 (16) −0.0020 (18) −0.0060 (16)
OW 0.154 (2) 0.0616 (15) 0.146 (2) −0.0265 (16) 0.073 (2) −0.0184 (15)

Geometric parameters (Å, °)

N1—C13 1.410 (3) C13—C14 1.386 (4)
N1—C7 1.421 (3) C13—C18 1.396 (3)
N1—C6 1.426 (3) C14—C15 1.373 (3)
C1—C6 1.377 (3) C14—H14A 0.9300
C1—C2 1.383 (4) C15—C16 1.401 (3)
C1—H1A 0.9300 C15—H15A 0.9300
N2—C19 1.324 (3) C16—C17 1.382 (3)
N2—C20 1.381 (3) C16—C19 1.464 (3)
C2—C3 1.369 (4) C17—C18 1.380 (3)
C2—H2B 0.9300 C17—H17A 0.9300
N3—C19 1.380 (3) C18—H18A 0.9300
N3—C25 1.381 (3) C20—C21 1.388 (3)
N3—C26 1.473 (3) C20—C25 1.398 (4)
C3—C4 1.365 (4) C21—C22 1.369 (4)
C3—H3A 0.9300 C21—H21A 0.9300
C4—C5 1.384 (4) C22—C23 1.401 (4)
C4—H4A 0.9300 C22—H22A 0.9300
C5—C6 1.388 (3) C23—C24 1.368 (4)
C5—H5A 0.9300 C23—H23A 0.9300
C7—C12 1.374 (4) C24—C25 1.397 (3)
C7—C8 1.380 (3) C24—H24A 0.9300
C8—C9 1.375 (4) C26—C27 1.511 (4)
C8—H8A 0.9300 C26—H26A 0.9700
C9—C10 1.356 (5) C26—H26B 0.9700
C9—H9A 0.9300 C27—H27A 0.9600
C10—C11 1.365 (5) C27—H27B 0.9600
C10—H10A 0.9300 C27—H27C 0.9600
C11—C12 1.378 (4) OW—HWB 0.8499
C11—H11A 0.9300 OW—HWA 0.8501
C12—H12A 0.9300
C13—N1—C7 119.5 (2) C13—C14—H14A 119.7
C13—N1—C6 120.7 (2) C14—C15—C16 121.4 (2)
C7—N1—C6 118.9 (2) C14—C15—H15A 119.3
C6—C1—C2 120.2 (3) C16—C15—H15A 119.3
C6—C1—H1A 119.9 C17—C16—C15 117.7 (2)
C2—C1—H1A 119.9 C17—C16—C19 124.3 (2)
C19—N2—C20 105.2 (2) C15—C16—C19 117.8 (2)
C3—C2—C1 120.4 (3) C18—C17—C16 121.4 (2)
C3—C2—H2B 119.8 C18—C17—H17A 119.3
C1—C2—H2B 119.8 C16—C17—H17A 119.3
C19—N3—C25 106.37 (19) C17—C18—C13 120.4 (2)
C19—N3—C26 129.6 (2) C17—C18—H18A 119.8
C25—N3—C26 123.6 (2) C13—C18—H18A 119.8
C4—C3—C2 119.9 (3) N2—C19—N3 112.5 (2)
C4—C3—H3A 120.0 N2—C19—C16 121.7 (2)
C2—C3—H3A 120.0 N3—C19—C16 125.7 (2)
C3—C4—C5 120.4 (3) N2—C20—C21 129.9 (2)
C3—C4—H4A 119.8 N2—C20—C25 110.1 (2)
C5—C4—H4A 119.8 C21—C20—C25 120.0 (2)
C4—C5—C6 119.9 (3) C22—C21—C20 118.2 (3)
C4—C5—H5A 120.1 C22—C21—H21A 120.9
C6—C5—H5A 120.1 C20—C21—H21A 120.9
C1—C6—C5 119.2 (2) C21—C22—C23 120.9 (3)
C1—C6—N1 120.6 (2) C21—C22—H22A 119.6
C5—C6—N1 120.2 (2) C23—C22—H22A 119.6
C12—C7—C8 119.1 (2) C24—C23—C22 122.6 (3)
C12—C7—N1 120.6 (2) C24—C23—H23A 118.7
C8—C7—N1 120.3 (2) C22—C23—H23A 118.7
C9—C8—C7 120.3 (3) C23—C24—C25 116.0 (3)
C9—C8—H8A 119.9 C23—C24—H24A 122.0
C7—C8—H8A 119.9 C25—C24—H24A 122.0
C10—C9—C8 120.4 (3) N3—C25—C24 131.8 (2)
C10—C9—H9A 119.8 N3—C25—C20 105.8 (2)
C8—C9—H9A 119.8 C24—C25—C20 122.4 (2)
C9—C10—C11 119.8 (3) N3—C26—C27 112.9 (2)
C9—C10—H10A 120.1 N3—C26—H26A 109.0
C11—C10—H10A 120.1 C27—C26—H26A 109.0
C10—C11—C12 120.6 (3) N3—C26—H26B 109.0
C10—C11—H11A 119.7 C27—C26—H26B 109.0
C12—C11—H11A 119.7 H26A—C26—H26B 107.8
C7—C12—C11 119.8 (3) C26—C27—H27A 109.5
C7—C12—H12A 120.1 C26—C27—H27B 109.5
C11—C12—H12A 120.1 H27A—C27—H27B 109.5
C14—C13—C18 118.6 (2) C26—C27—H27C 109.5
C14—C13—N1 121.8 (2) H27A—C27—H27C 109.5
C18—C13—N1 119.6 (2) H27B—C27—H27C 109.5
C15—C14—C13 120.5 (2) HWB—OW—HWA 106.9
C15—C14—H14A 119.7
C6—C1—C2—C3 −0.9 (4) C19—C16—C17—C18 −176.2 (2)
C1—C2—C3—C4 0.7 (5) C16—C17—C18—C13 0.4 (4)
C2—C3—C4—C5 0.7 (4) C14—C13—C18—C17 0.5 (4)
C3—C4—C5—C6 −1.8 (4) N1—C13—C18—C17 −178.8 (2)
C2—C1—C6—C5 −0.3 (4) C20—N2—C19—N3 0.0 (3)
C2—C1—C6—N1 −178.8 (3) C20—N2—C19—C16 −179.3 (2)
C4—C5—C6—C1 1.6 (4) C25—N3—C19—N2 −0.2 (3)
C4—C5—C6—N1 −179.8 (3) C26—N3—C19—N2 172.0 (2)
C13—N1—C6—C1 −136.8 (3) C25—N3—C19—C16 179.0 (2)
C7—N1—C6—C1 32.2 (4) C26—N3—C19—C16 −8.7 (4)
C13—N1—C6—C5 44.7 (4) C17—C16—C19—N2 142.4 (3)
C7—N1—C6—C5 −146.3 (2) C15—C16—C19—N2 −32.3 (3)
C13—N1—C7—C12 −130.9 (3) C17—C16—C19—N3 −36.8 (4)
C6—N1—C7—C12 59.9 (3) C15—C16—C19—N3 148.5 (2)
C13—N1—C7—C8 50.7 (3) C19—N2—C20—C21 179.5 (3)
C6—N1—C7—C8 −118.5 (3) C19—N2—C20—C25 0.2 (3)
C12—C7—C8—C9 −0.2 (4) N2—C20—C21—C22 −178.5 (3)
N1—C7—C8—C9 178.2 (2) C25—C20—C21—C22 0.6 (4)
C7—C8—C9—C10 −0.5 (4) C20—C21—C22—C23 −0.6 (5)
C8—C9—C10—C11 1.0 (5) C21—C22—C23—C24 −0.2 (5)
C9—C10—C11—C12 −0.7 (5) C22—C23—C24—C25 0.8 (5)
C8—C7—C12—C11 0.5 (4) C19—N3—C25—C24 −179.4 (3)
N1—C7—C12—C11 −177.9 (3) C26—N3—C25—C24 7.8 (4)
C10—C11—C12—C7 −0.1 (5) C19—N3—C25—C20 0.4 (3)
C7—N1—C13—C14 −137.3 (3) C26—N3—C25—C20 −172.5 (2)
C6—N1—C13—C14 31.7 (4) C23—C24—C25—N3 178.9 (3)
C7—N1—C13—C18 42.1 (3) C23—C24—C25—C20 −0.8 (4)
C6—N1—C13—C18 −149.0 (2) N2—C20—C25—N3 −0.4 (3)
C18—C13—C14—C15 −0.3 (4) C21—C20—C25—N3 −179.7 (2)
N1—C13—C14—C15 179.0 (2) N2—C20—C25—C24 179.4 (2)
C13—C14—C15—C16 −0.9 (4) C21—C20—C25—C24 0.0 (4)
C14—C15—C16—C17 1.8 (4) C19—N3—C26—C27 110.2 (3)
C14—C15—C16—C19 176.8 (2) C25—N3—C26—C27 −78.7 (3)
C15—C16—C17—C18 −1.6 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
OW—HWB···N2 0.85 2.50 2.903 (3) 110
OW—HWA···N2 0.85 2.49 2.903 (3) 111
C24—H24A···OWi 0.93 2.43 3.352 (4) 173

Symmetry codes: (i) x, y−1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BQ2268).

References

  1. Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
  2. Enraf–Nonius (1985). CAD-4 Software Enraf–Nonius, Delft, The Netherlands.
  3. Harms, K. & Wocadlo, S. (1995). XCAD4 University of Marburg, Germany.
  4. Kakimoto, M., Ge, Z. Y., Hayakawa, T., Ando, S. & Ueda, M. (2008). Adv. Funct. Mater. 18, 584–590.
  5. North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Vinodkumar, R., Vaidya, S. D., Kumar, B. V. S., Bhise, U. N. & Mashelkar, U. C. (2008). ARKIVOC, 14, 37–49.

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/S160053681100119X/bq2268sup1.cif

e-67-0o417-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681100119X/bq2268Isup2.hkl

e-67-0o417-Isup2.hkl (197.2KB, hkl)

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


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