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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 16;68(Pt 6):m767. doi: 10.1107/S1600536812020910

Bis(2-aminomethyl-1H-benzimidazole-κ2 N 2,N 3)bis­(nitrato-κO)copper(II)

Jing Zhao a,b, Heng Zhang c, Xueliang Zhai c, Guoyi Zhu a,*
PMCID: PMC3379102  PMID: 22719323

Abstract

In the title compound, [Cu(NO3)2(C8H9N3)2], the CuII atom, lying on an inversion center, has a distorted octa­hedral coordination environment defined by four N atoms from two chelating 2-amino­methyl-1H-benzimidazole ligands and two O atoms from two monodentate nitrate anions. In the crystal, N—H⋯O hydrogen bonds link the complex mol­ecules into a three-dimensional network. An intra­molecular N—H⋯O hydrogen bond is also observed.

Related literature  

For the synthesis of the 2-(2-amino­meth­yl)benzimidazole ligand, see: Pascaly et al. (2001). For the structures and properties of transition metal complexes with 2-(2-amino­meth­yl)benzimidazole ligands, see: Gable et al. (1996); Gómez-Segura et al. (2006); He et al. (2003); Jiang et al. (2004).graphic file with name e-68-0m767-scheme1.jpg

Experimental  

Crystal data  

  • [Cu(NO3)2(C8H9N3)2]

  • M r = 481.93

  • Trigonal, Inline graphic

  • a = 24.6913 (8) Å

  • c = 7.9620 (5) Å

  • V = 4203.8 (4) Å3

  • Z = 9

  • Mo Kα radiation

  • μ = 1.23 mm−1

  • T = 184 K

  • 0.34 × 0.21 × 0.11 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.681, T max = 0.877

  • 7196 measured reflections

  • 1833 independent reflections

  • 1764 reflections with I > 2σ(I)

  • R int = 0.015

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.023

  • wR(F 2) = 0.063

  • S = 1.04

  • 1833 reflections

  • 142 parameters

  • H-atom parameters constrained

  • Δρmax = 0.52 e Å−3

  • Δρmin = −0.23 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; 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 datablock(s) I, global. DOI: 10.1107/S1600536812020910/hy2548sup1.cif

e-68-0m767-sup1.cif (15.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020910/hy2548Isup2.hkl

e-68-0m767-Isup2.hkl (90.6KB, 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
N3—H3A⋯O1i 0.92 2.42 3.266 (2) 153
N3—H3A⋯O3i 0.92 2.37 3.0521 (17) 131
N3—H3B⋯O1ii 0.92 2.33 3.1036 (19) 142
N2—H2⋯O3iii 0.88 2.50 3.0276 (18) 119
N2—H2⋯O3iv 0.88 2.40 3.0823 (18) 134
N2—H2⋯O2iii 0.88 2.20 2.8901 (17) 135

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

Acknowledgments

This work was supported by the Youth Foundation of Hebei Normal University (No. L2006Q20).

supplementary crystallographic information

Comment

Benzimidazole is of considerable interest as a ligand for transition metal ions. Some of their polyfunctional derivatives have been proved to possess extensive biological activities (Gómez-Segura et al., 2006). Therefore, substituted benzimidazoles have attracted interest of various research groups, especially the substitution at 1, 2 and 5 positions of the benzimidazole ring is very important for their coordination behavior. The 2-(2-aminomethyl)-1H-benzimidazole (AMBI) ligand is a suitable model system for compounds of this sort, which is a bidentate ligand and can chelate a 3d metal ion through two nitrogen atoms of the pendant aminomethyl group and the imidazole ring (Gable et al., 1996; He et al., 2003; Jiang et al., 2004). Moreover, AMBI possesses a larger conjugated π-system and a nitrogen electron-donor of the secondary amine group, which has an important effect on the structures and functions of the complexes. On the other hand, metalloproteins that contain Cu are widespread. Characterization of model Cu complexes that mimic Cu proteins has led to a better understanding of the chemistry of Cu in biological systems. A new copper(II) complex with AMBI, which is reported in this paper, may be of interest with respect to both of the above-mentioned areas.

In the title compound, as shown in Fig. 1, two bidentate AMBI ligands are coordinated to the CuII atom via two N atoms and two nitrate anions are coordinated to the CuII atom via one O atom. The coordination geometry around the CuII atom, which lies on an inversion center, is distorted octahedral, with a bite angle of 83.84 (5)° for two bidentate ligands. The other cis bond angles at the CuII atom fall in the range of 80.71 (5)–99.29 (5)° and the trans bond angles are 180°, suggesting a significant deviation from a perfect octahedral coordination. The Cu—N bond lengths are 1.9839 (12) and 2.0244 (12) Å, with an average of 2.0042 (12) Å. The Cu—O bond length is 2.5870 (12) Å. Extensive N—H···O hydrogen bonds in the crystal, as shown in Fig. 2 and Table 1, link the complex molecules into a three-dimensional network.

Experimental

The title compound was prepared by adding a methanol-water solution (4:1 v/v, 5 ml) of Cu(NO3)2.3H2O (0.1 mmol) to a methanol solution (5 ml) of 2-(2-aminomethyl)benzimidazole (0.2 mmol) (Pascaly et al., 2001). The blue mixture was stirred at room temperature for 4 h and then filtered. Purple crystals suitable for X-ray diffraction were obtained by slow evaporation of the solvent after several days. Analysis, calculated for C16H18CuN8O6: C 39.88, H 3.76, N 23.25%; found: C 39.92, H 3.75, N 23.30%.

Refinement

H atoms bonded to C and N atoms were positioned geometrically and refined as riding atoms, with C—H = 0.95 (aromatic), 0.99 (CH2) and N—H = 0.88 (NH), 0.92 (NH2) Å and with Uiso(H) = 1.2Ueq(C,N).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title complex, with displacement ellipsoids drawn at the 30% probability level. [Symmetry code: (A) -x+5/3, -y+1/3, -z+1/3.]

Fig. 2.

Fig. 2.

The packing diagram viewed along the c axis.

Crystal data

[Cu(NO3)2(C8H9N3)2] Dx = 1.713 Mg m3
Mr = 481.93 Mo Kα radiation, λ = 0.71073 Å
Trigonal, R3 Cell parameters from 5478 reflections
Hall symbol: -R 3 θ = 2.7–26.0°
a = 24.6913 (8) Å µ = 1.23 mm1
c = 7.9620 (5) Å T = 184 K
V = 4203.8 (4) Å3 Block, purple
Z = 9 0.34 × 0.21 × 0.11 mm
F(000) = 2223

Data collection

Bruker APEXII CCD diffractometer 1833 independent reflections
Radiation source: fine-focus sealed tube 1764 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.015
φ and ω scans θmax = 26.0°, θmin = 1.7°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −27→30
Tmin = 0.681, Tmax = 0.877 k = −25→30
7196 measured reflections l = −9→8

Refinement

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)] = 0.023 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.063 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0358P)2 + 6.4022P] where P = (Fo2 + 2Fc2)/3
1833 reflections (Δ/σ)max = 0.001
142 parameters Δρmax = 0.52 e Å3
0 restraints Δρmin = −0.23 e Å3

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
Cu1 0.8333 0.1667 0.1667 0.01942 (10)
O1 0.85026 (6) 0.28108 (7) 0.46236 (18) 0.0427 (3)
O2 0.89291 (6) 0.22280 (5) 0.43740 (16) 0.0339 (3)
O3 0.94763 (5) 0.31844 (5) 0.52565 (15) 0.0321 (3)
N1 0.84262 (6) 0.24335 (6) 0.05919 (15) 0.0205 (3)
N2 0.89615 (6) 0.31981 (6) −0.12266 (16) 0.0241 (3)
H2 0.9235 0.3420 −0.2009 0.029*
N3 0.90693 (6) 0.18332 (6) 0.01943 (15) 0.0222 (3)
H3A 0.9417 0.1958 0.0856 0.027*
H3B 0.8986 0.1469 −0.0339 0.027*
N4 0.89671 (6) 0.27418 (6) 0.47583 (16) 0.0249 (3)
C1 0.92024 (7) 0.23207 (7) −0.10792 (19) 0.0237 (3)
H1A 0.9053 0.2126 −0.2196 0.028*
H1B 0.9658 0.2615 −0.1149 0.028*
C2 0.88719 (7) 0.26609 (7) −0.05640 (18) 0.0207 (3)
C3 0.82031 (7) 0.28550 (7) 0.06771 (18) 0.0212 (3)
C4 0.77224 (8) 0.28515 (8) 0.1601 (2) 0.0283 (3)
H4 0.7479 0.2524 0.2367 0.034*
C5 0.76134 (8) 0.33433 (8) 0.1360 (2) 0.0326 (4)
H5 0.7284 0.3348 0.1967 0.039*
C6 0.79714 (9) 0.38357 (8) 0.0253 (2) 0.0349 (4)
H6 0.7886 0.4169 0.0140 0.042*
C7 0.84461 (8) 0.38431 (8) −0.0675 (2) 0.0319 (4)
H7 0.8693 0.4176 −0.1426 0.038*
C8 0.85467 (7) 0.33414 (7) −0.04615 (18) 0.0232 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.01800 (15) 0.01646 (14) 0.02290 (16) 0.00795 (10) 0.00401 (9) 0.00463 (9)
O1 0.0359 (7) 0.0535 (8) 0.0510 (8) 0.0317 (7) −0.0132 (6) −0.0165 (6)
O2 0.0334 (6) 0.0253 (6) 0.0454 (7) 0.0165 (5) −0.0137 (5) −0.0077 (5)
O3 0.0276 (6) 0.0252 (6) 0.0372 (7) 0.0086 (5) −0.0043 (5) −0.0033 (5)
N1 0.0208 (6) 0.0184 (6) 0.0215 (6) 0.0092 (5) 0.0021 (5) 0.0019 (5)
N2 0.0250 (7) 0.0214 (6) 0.0236 (6) 0.0100 (5) 0.0049 (5) 0.0066 (5)
N3 0.0199 (6) 0.0210 (6) 0.0245 (6) 0.0094 (5) 0.0017 (5) 0.0024 (5)
N4 0.0272 (7) 0.0284 (7) 0.0207 (6) 0.0151 (6) −0.0016 (5) 0.0002 (5)
C1 0.0240 (7) 0.0245 (7) 0.0220 (7) 0.0117 (6) 0.0050 (6) 0.0037 (6)
C2 0.0200 (7) 0.0194 (7) 0.0188 (7) 0.0069 (6) −0.0004 (5) 0.0010 (5)
C3 0.0223 (7) 0.0182 (7) 0.0221 (7) 0.0094 (6) −0.0032 (6) −0.0008 (5)
C4 0.0279 (8) 0.0276 (8) 0.0308 (8) 0.0150 (7) 0.0040 (6) 0.0037 (6)
C5 0.0332 (9) 0.0338 (9) 0.0376 (9) 0.0218 (8) 0.0015 (7) −0.0005 (7)
C6 0.0407 (10) 0.0280 (8) 0.0437 (10) 0.0229 (8) −0.0037 (8) 0.0016 (7)
C7 0.0354 (9) 0.0239 (8) 0.0362 (9) 0.0148 (7) −0.0002 (7) 0.0071 (7)
C8 0.0222 (7) 0.0200 (7) 0.0241 (7) 0.0081 (6) −0.0031 (6) 0.0007 (6)

Geometric parameters (Å, º)

Cu1—N1 1.9839 (12) C1—C2 1.492 (2)
Cu1—N3 2.0244 (12) C1—H1A 0.9900
Cu1—O2 2.5870 (12) C1—H1B 0.9900
O1—N4 1.2454 (18) C3—C4 1.393 (2)
O2—N4 1.2621 (17) C3—C8 1.402 (2)
O3—N4 1.2483 (17) C4—C5 1.382 (2)
N1—C2 1.3250 (19) C4—H4 0.9500
N1—C3 1.4016 (19) C5—C6 1.401 (3)
N2—C2 1.3390 (19) C5—H5 0.9500
N2—C8 1.381 (2) C6—C7 1.378 (3)
N2—H2 0.8800 C6—H6 0.9500
N3—C1 1.4798 (19) C7—C8 1.390 (2)
N3—H3A 0.9200 C7—H7 0.9500
N3—H3B 0.9200
N1—Cu1—N1i 179.999 (1) N3—C1—H1A 110.1
N1—Cu1—N3 83.84 (5) C2—C1—H1A 110.1
N1i—Cu1—N3 96.16 (5) N3—C1—H1B 110.1
N1—Cu1—N3i 96.16 (5) C2—C1—H1B 110.1
N1i—Cu1—N3i 83.84 (5) H1A—C1—H1B 108.4
N3—Cu1—N3i 180.00 (5) N1—C2—N2 112.60 (13)
N1—Cu1—O2 94.86 (4) N1—C2—C1 121.64 (13)
N1i—Cu1—O2 85.14 (4) N2—C2—C1 125.70 (13)
N3—Cu1—O2 99.29 (5) C4—C3—N1 132.16 (14)
N3i—Cu1—O2 80.71 (5) C4—C3—C8 119.72 (14)
N4—O2—Cu1 118.50 (9) N1—C3—C8 108.09 (13)
C2—N1—C3 105.70 (12) C5—C4—C3 117.45 (15)
C2—N1—Cu1 112.29 (10) C5—C4—H4 121.3
C3—N1—Cu1 141.90 (10) C3—C4—H4 121.3
C2—N2—C8 107.67 (12) C4—C5—C6 122.28 (16)
C2—N2—H2 126.2 C4—C5—H5 118.9
C8—N2—H2 126.2 C6—C5—H5 118.9
C1—N3—Cu1 111.94 (9) C7—C6—C5 120.84 (15)
C1—N3—H3A 109.2 C7—C6—H6 119.6
Cu1—N3—H3A 109.2 C5—C6—H6 119.6
C1—N3—H3B 109.2 C6—C7—C8 116.89 (15)
Cu1—N3—H3B 109.2 C6—C7—H7 121.6
H3A—N3—H3B 107.9 C8—C7—H7 121.6
O1—N4—O3 120.07 (13) N2—C8—C7 131.30 (15)
O1—N4—O2 120.38 (14) N2—C8—C3 105.93 (13)
O3—N4—O2 119.55 (13) C7—C8—C3 122.77 (15)
N3—C1—C2 107.95 (12)

Symmetry code: (i) −x+5/3, −y+1/3, −z+1/3.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N3—H3A···O1ii 0.92 2.42 3.266 (2) 153
N3—H3A···O3ii 0.92 2.37 3.0521 (17) 131
N3—H3B···O1i 0.92 2.33 3.1036 (19) 142
N2—H2···O3iii 0.88 2.50 3.0276 (18) 119
N2—H2···O3iv 0.88 2.40 3.0823 (18) 134
N2—H2···O2iii 0.88 2.20 2.8901 (17) 135

Symmetry codes: (i) −x+5/3, −y+1/3, −z+1/3; (ii) −y+4/3, xy−1/3, z−1/3; (iii) −x+y+5/3, −x+4/3, z−2/3; (iv) x, y, z−1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HY2548).

References

  1. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Gable, R. W., Hartshorn, R. M., Mcfadyen, W. D. & Nunno, L. (1996). Aust. J. Chem. 49, 625–632.
  3. Gómez-Segura, J., Prieto, M. J., Font-Bardia, M., Solans, X. & Moreno, V. (2006). Inorg. Chem. 45, 10031–10033. [DOI] [PubMed]
  4. He, Y., Kou, H.-Z., Wang, R.-J. & Li, Y.-D. (2003). Transition Met. Chem. 28, 464–467.
  5. Jiang, Y.-B., Kou, H.-Z., Gao, F. & Wang, R.-J. (2004). Acta Cryst. C60, m261–m262. [DOI] [PubMed]
  6. Pascaly, M., Duda, M., Schweppe, F., Zurlinden, K., Müller, F. K. & Krebs, B. (2001). J. Chem. Soc. Dalton Trans. pp. 828–837.
  7. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812020910/hy2548sup1.cif

e-68-0m767-sup1.cif (15.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020910/hy2548Isup2.hkl

e-68-0m767-Isup2.hkl (90.6KB, hkl)

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


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