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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Feb 22;64(Pt 3):o621–o622. doi: 10.1107/S1600536808004893

1,3-Bis(3-phenyl­prop­yl)-1H-benz­imidazole-2(3H)-tellurone

Şerife Pınar Yalçın a, Mehmet Akkurt a,*, Ülkü Yılmaz b, Hasan Küçükbay b, Orhan Büyükgüngör c
PMCID: PMC2960818  PMID: 21201955

Abstract

The title compound, C25H26N2Te, was synthesized from bis­[1,3-bis­(3-phenyl­prop­yl)benzimidazolidin-2-yl­idene] and Te in a toluene solution. The molecule possesses a twofold rotation axis passing through the Te atom and the center of the benzimidazole ring system. The benzimidazole ring system makes an angle of 67.9 (4)° with the phenyl rings.

Related literature

For related literature, see: Akkurt et al. (2004a ,b , 2005); Aydın et al. (1999); Chakravorty et al. (1985); Karaca et al. (2005); Lappert (1988); Lappert et al. (1980); Roeterdink et al. (1983); Türktekin et al. (2004); İngeç et al. (1999); Närhi et al. (2004); Sadekov et al. (1998); Singh et al. (2006).graphic file with name e-64-0o621-scheme1.jpg

Experimental

Crystal data

  • C25H26N2Te

  • M r = 482.08

  • Tetragonal, Inline graphic

  • a = 10.6004 (2) Å

  • c = 20.4365 (6) Å

  • V = 2296.42 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.31 mm−1

  • T = 296 K

  • 0.54 × 0.48 × 0.39 mm

Data collection

  • Stoe IPDSII diffractometer

  • Absorption correction: integration (X-RED32; Stoe & Cie, 2002) T min = 0.539, T max = 0.630

  • 28301 measured reflections

  • 2264 independent reflections

  • 2166 reflections with I > 2σ(I)

  • R int = 0.049

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.105

  • S = 1.09

  • 2264 reflections

  • 99 parameters

  • 3 restraints

  • H-atom parameters constrained

  • Δρmax = 0.92 e Å−3

  • Δρmin = −0.48 e Å−3

  • Absolute structure: Flack (1983), 889 Friedel pairs

  • Flack parameter: 0.01 (6)

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808004893/ez2117sup1.cif

e-64-0o621-sup1.cif (18.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808004893/ez2117Isup2.hkl

e-64-0o621-Isup2.hkl (109.1KB, hkl)

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

Table 1. Selected bond lengths (Å).

Te1—C1 2.058 (4)

Acknowledgments

The authors acknowledge the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDSII diffractometer (purchased under grant F.279 of the University Research Fund). ÜY and HK also thank the İnönü University Research Fund (BAPB-2006–41) for financial support of this study.

supplementary crystallographic information

Comment

Electron-rich olefins are powerful reducing agents (Lappert, 1988). It is known that the ultimate oxidation products of electron-rich olefins with air are ureas; sulfur and selenium react similarly to form the corresponding analogues (Roeterdink et al., 1983; Lappert et al., 1980). The conversion of an electron-rich olefin into a tellurourea has a parallel in these known olefin reactions (Lappert et al., 1980). There are extensive studies of cyclic ureas containing imidazolidine groups, including their X-ray crystal structures. However, there is no example of an X-ray crystal structure study for the cyclic tellurourea containing a benzimidazole group. The objective of this study was to elucidate the first crystal structure of such a cyclic tellurourea and compare the results to the corresponding analogues contain sulfur (İngeç et al., 1999) and selenium (Aydın et al., 1999; Akkurt et al., 2004a).

The molecular structure of the title compound (I) is shown in Fig. 1. The molecule has a twofold screw axis through the midpoints of the C2—C2a and C4—C4a bonds and containing the atoms Te1 and C1 of the benzimidazole ring. The Te—C single bond length generally varies between 2.120 and 2.170 Å depending on the electron releasing effect of the ligand bonding to Te atom (Lappert et al., 1980; Sadekov et al., 1998; Närhi et al., 2004; Singh et al., 2006). In the title compound (I), the Te—C bond length [2.058 (4) Å] is short, which agrees with the results reported by Lappert et al. (1980). Tellurourea metal complexes may be described in terms of the resonance hybrids as shown in the scheme 2. For this reason, the Te?C bond may have partial double bond character.

All the geometric parameters of (I) are comparable with those in related compounds (Akkurt et al., 2004b; Akkurt et al., 2005; Türktekin et al., 2004, Karaca et al., 2005).

In the title molecule, the benzimidazole ring system (C1—C3/N1/C1a—C3a/N1a) is essentially planar, with maximum deviations of 0.007 (5) Å for C2 and -0.007 (5) Å for C2a. The symmetry-related phenyl rings (C8–C13 and C8a–C13a) are oriented at angles of 67.9 (4)° to the plane of the benzimidazole ring system.

Experimental

A mixture of bis(1,3-di(3-phenylpropyl)benzimidazolidine-2-ylidene) (0.55 g; 0.78 mmol) and tellurium (0.22 g; 1.72 mmol) in toluene (10 ml) was heated under reflux for 2 h. The mixture was then filtered to remove unreacted tellurium and upon cooling the filtrate to 253 K, light yellow crystals of the title compound were obtained. (Yield: 0.54 g, 72%; m.p.: 390–391 K). 1H-NMR (CDCl3): δ 2.25 (q, 4H, CH2), 2.83 (t, 4H, CH2), 4.53 (t, 4H, N—CH2), 7.14–7.24 (m, 14H, Ar—H). 13C-NMR (CDCl3): δ 29.74, 32.99, 49.25, 110.26, 123.61, 126.20, 128.38, 128.50, 133.93, 140.73, 144.18. Analysis calculated for C25H26N2Te: C 62.29, H 5.40, N 5.82%. Found: C 62.52, H 5.50, N 5.82%.

Refinement

The H atoms were placed in calculated positions and refined using a riding model with C—H in the range 0.93–0.97 Å and Uiso(H) = 1.2Ueq(C). Atoms C8, C9 and C13 in the phenyl ring appear to have unresolved disorder, so the distances C8—C9, C8—C13 and C9···C13 were restrained by SHELXL DFIX instructions [C8—C9 = 1.370 (12), C8—C13 = 1.336 (14) and C9···C13 = 2.229 (14) Å].

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound (I) with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 30% probability level. [Symmetry code: (a) -y + 1, -x + 1, -z + 3/2.]

Fig. 2.

Fig. 2.

The resonance hybrids of tellurourea metal complexes (Lappert et al., 1980).

Crystal data

C25H26N2Te Z = 4
Mr = 482.08 F000 = 968
Tetragonal, P41212 Dx = 1.394 Mg m3
Hall symbol: P 4abw 2nw Mo Kα radiation λ = 0.71073 Å
a = 10.6004 (2) Å Cell parameters from 55040 reflections
b = 10.6004 (2) Å θ = 1.9–27.2º
c = 20.4365 (6) Å µ = 1.31 mm1
α = 90º T = 296 K
β = 90º Block, light yellow
γ = 90º 0.54 × 0.48 × 0.39 mm
V = 2296.42 (9) Å3

Data collection

Stoe IPDSII diffractometer 2264 independent reflections
Monochromator: plane graphite 2166 reflections with I > 2σ(I)
Detector resolution: 6.67 pixels mm-1 Rint = 0.049
T = 296 K θmax = 26.0º
ω scans θmin = 2.2º
Absorption correction: integration(X-RED32; Stoe & Cie, 2002) h = −12→13
Tmin = 0.539, Tmax = 0.630 k = −13→13
28301 measured reflections l = −25→25

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.037   w = 1/[σ2(Fo2) + (0.0574P)2 + 1.6917P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.105 (Δ/σ)max < 0.001
S = 1.09 Δρmax = 0.92 e Å3
2264 reflections Δρmin = −0.48 e Å3
99 parameters Extinction correction: none
3 restraints Absolute structure: Flack (1983), 889 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.01 (6)
Secondary atom site location: difference Fourier map

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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
Te1 0.13779 (3) 0.86221 (3) 0.75000 0.0633 (1)
N1 0.3555 (4) 0.6989 (4) 0.79960 (17) 0.0585 (11)
C1 0.2751 (4) 0.7249 (4) 0.75000 0.0550 (14)
C2 0.4349 (5) 0.6006 (5) 0.7811 (2) 0.0653 (17)
C3 0.5312 (6) 0.5400 (6) 0.8141 (3) 0.084 (2)
C4 0.5917 (7) 0.4441 (7) 0.7828 (4) 0.101 (3)
C5 0.3626 (6) 0.7656 (5) 0.8618 (2) 0.0630 (16)
C6 0.4521 (5) 0.8761 (5) 0.8597 (2) 0.0677 (16)
C7 0.4498 (6) 0.9471 (5) 0.9247 (3) 0.0723 (19)
C8 0.5329 (9) 1.0605 (7) 0.9284 (5) 0.1219 (15)
C9 0.4939 (9) 1.1694 (7) 0.9583 (5) 0.1219 (15)
C10 0.5698 (9) 1.2703 (7) 0.9670 (5) 0.1219 (15)
C11 0.6886 (9) 1.2679 (7) 0.9451 (5) 0.1219 (15)
C12 0.7332 (10) 1.1639 (7) 0.9160 (5) 0.1219 (15)
C13 0.6524 (9) 1.0587 (7) 0.9076 (5) 0.1219 (15)
H3 0.55390 0.56380 0.85620 0.1020*
H4 0.65670 0.40140 0.80390 0.1210*
H5A 0.38990 0.70730 0.89550 0.0750*
H5B 0.27910 0.79550 0.87340 0.0750*
H6A 0.42790 0.93270 0.82460 0.0810*
H6B 0.53690 0.84620 0.85100 0.0810*
H7A 0.36370 0.97330 0.93340 0.0870*
H7B 0.47420 0.88920 0.95920 0.0870*
H9 0.41130 1.17400 0.97330 0.1460*
H10 0.53940 1.34170 0.98830 0.1460*
H11 0.74010 1.33830 0.95000 0.1460*
H12 0.81630 1.16070 0.90150 0.1460*
H13 0.68330 0.98660 0.88720 0.1460*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Te1 0.0682 (2) 0.0682 (2) 0.0535 (2) 0.0114 (2) 0.0052 (2) 0.0052 (2)
N1 0.071 (2) 0.059 (2) 0.0454 (17) −0.002 (2) −0.0194 (17) −0.0106 (15)
C1 0.061 (2) 0.061 (2) 0.043 (3) −0.002 (2) −0.004 (2) −0.004 (2)
C2 0.073 (3) 0.061 (3) 0.062 (3) 0.003 (2) −0.017 (2) −0.017 (2)
C3 0.084 (4) 0.085 (4) 0.084 (3) 0.012 (3) −0.039 (3) −0.015 (3)
C4 0.082 (4) 0.085 (5) 0.136 (6) 0.024 (4) −0.031 (4) −0.020 (4)
C5 0.085 (3) 0.065 (3) 0.039 (2) −0.001 (3) −0.008 (2) −0.0117 (18)
C6 0.085 (3) 0.064 (3) 0.054 (2) −0.007 (3) −0.014 (2) −0.008 (2)
C7 0.091 (4) 0.062 (3) 0.064 (3) 0.005 (3) −0.016 (3) −0.021 (2)
C8 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)
C9 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)
C10 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)
C11 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)
C12 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)
C13 0.132 (3) 0.0736 (16) 0.160 (3) −0.0065 (19) −0.034 (3) −0.0275 (19)

Geometric parameters (Å, °)

Te1—C1 2.058 (4) C11—C12 1.339 (12)
N1—C1 1.353 (5) C12—C13 1.417 (12)
N1—C2 1.392 (7) C3—H3 0.9300
N1—C5 1.457 (6) C4—H4 0.9300
C2—C3 1.382 (8) C5—H5A 0.9700
C2—C2i 1.378 (6) C5—H5B 0.9700
C3—C4 1.362 (10) C6—H6A 0.9700
C4—C4i 1.444 (11) C6—H6B 0.9700
C5—C6 1.508 (8) C7—H7A 0.9700
C6—C7 1.527 (7) C7—H7B 0.9700
C7—C8 1.492 (10) C9—H9 0.9300
C8—C9 1.370 (12) C10—H10 0.9300
C8—C13 1.336 (14) C11—H11 0.9300
C9—C10 1.350 (12) C12—H12 0.9300
C10—C11 1.337 (14) C13—H13 0.9300
Te1···H5B 3.0200 H5A···H7B 2.4900
Te1···H3ii 3.1700 H5B···Te1 3.0200
Te1···H7Bii 3.2900 H5B···H7A 2.4200
Te1···H10iii 3.3200 H6A···H7Bii 2.5900
Te1···H3iv 3.1700 H6B···C13 2.8100
Te1···H7Biv 3.2900 H6B···H13 2.2700
Te1···H10v 3.3200 H7A···H5B 2.4200
Te1···H5Bi 3.0200 H7A···H9 2.3300
C3···H5A 2.8600 H7A···C4iv 3.0900
C4···H7Avi 3.0900 H7A···H4iv 2.5800
C5···H3 2.9500 H7B···H5A 2.4900
C6···H13 2.7700 H7B···Te1vii 3.2900
C13···H6B 2.8100 H7B···H6Avii 2.5900
H3···C5 2.9500 H7B···Te1vi 3.2900
H3···H5A 2.4500 H9···H7A 2.3300
H3···Te1vii 3.1700 H10···Te1viii 3.3200
H3···Te1vi 3.1700 H10···Te1ix 3.3200
H4···H7Avi 2.5800 H13···C6 2.7700
H5A···C3 2.8600 H13···H6B 2.2700
H5A···H3 2.4500
C1—N1—C2 109.3 (3) N1—C5—H5A 109.00
C1—N1—C5 126.0 (4) N1—C5—H5B 109.00
C2—N1—C5 124.7 (4) C6—C5—H5A 109.00
Te1—C1—N1 126.1 (2) C6—C5—H5B 109.00
Te1—C1—N1i 126.1 (2) H5A—C5—H5B 108.00
N1—C1—N1i 107.8 (4) C5—C6—H6A 110.00
N1—C2—C3 131.5 (4) C5—C6—H6B 110.00
N1—C2—C2i 106.9 (4) C7—C6—H6A 110.00
C2i—C2—C3 121.7 (5) C7—C6—H6B 110.00
C2—C3—C4 117.8 (6) H6A—C6—H6B 108.00
C3—C4—C4i 120.6 (7) C6—C7—H7A 108.00
N1—C5—C6 112.6 (4) C6—C7—H7B 108.00
C5—C6—C7 110.4 (4) C8—C7—H7A 108.00
C6—C7—C8 115.6 (6) C8—C7—H7B 108.00
C7—C8—C9 121.6 (8) H7A—C7—H7B 107.00
C7—C8—C13 122.1 (7) C8—C9—H9 118.00
C9—C8—C13 116.1 (8) C10—C9—H9 118.00
C8—C9—C10 123.1 (9) C9—C10—H10 120.00
C9—C10—C11 120.2 (8) C11—C10—H10 120.00
C10—C11—C12 119.8 (8) C10—C11—H11 120.00
C11—C12—C13 119.2 (9) C12—C11—H11 120.00
C8—C13—C12 121.6 (8) C11—C12—H12 120.00
C2—C3—H3 121.00 C13—C12—H12 120.00
C4—C3—H3 121.00 C8—C13—H13 119.00
C3—C4—H4 120.00 C12—C13—H13 119.00
C4i—C4—H4 120.00
C2—N1—C1—Te1 −179.6 (3) C2i—C2—C3—C4 0.8 (9)
C5—N1—C1—Te1 −1.9 (7) C2—C3—C4—C4i 0.3 (10)
C2—N1—C1—N1i 0.4 (5) C3—C4—C4i—C3i −0.8 (11)
C5—N1—C1—N1i 178.1 (4) N1—C5—C6—C7 176.6 (4)
C1—N1—C2—C3 −179.6 (6) C5—C6—C7—C8 −178.9 (6)
C5—N1—C2—C3 2.7 (9) C6—C7—C8—C9 139.2 (8)
C1—N1—C2—C2i −1.1 (5) C6—C7—C8—C13 −46.2 (11)
C5—N1—C2—C2i −178.8 (5) C7—C8—C9—C10 174.7 (9)
C1—N1—C5—C6 −89.3 (6) C13—C8—C9—C10 −0.1 (15)
C2—N1—C5—C6 88.1 (6) C7—C8—C13—C12 −175.0 (9)
N1—C2—C3—C4 179.1 (6) C9—C8—C13—C12 −0.2 (15)
N1—C2—C2i—C3i 180.0 (5) C8—C9—C10—C11 1.1 (16)
C3—C2—C2i—N1i 180.0 (5) C9—C10—C11—C12 −1.7 (15)
C3—C2—C2i—C3i −1.3 (8) C10—C11—C12—C13 1.4 (15)
N1—C2—C2i—N1i 1.3 (6) C11—C12—C13—C8 −0.4 (15)

Symmetry codes: (i) −y+1, −x+1, −z+3/2; (ii) y−1/2, −x+3/2, z−1/4; (iii) y−3/2, −x+3/2, z−1/4; (iv) x−1/2, −y+3/2, −z+7/4; (v) x−1/2, −y+5/2, −z+7/4; (vi) x+1/2, −y+3/2, −z+7/4; (vii) −y+3/2, x+1/2, z+1/4; (viii) −y+3/2, x+3/2, z+1/4; (ix) x+1/2, −y+5/2, −z+7/4.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: EZ2117).

References

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Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808004893/ez2117sup1.cif

e-64-0o621-sup1.cif (18.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808004893/ez2117Isup2.hkl

e-64-0o621-Isup2.hkl (109.1KB, hkl)

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


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