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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):m27. doi: 10.1107/S1600536810049421

The azide-bridged mixed-valent cobalt(II,III) compound [(CH3)3NH]2[CoIICo2 III(N3)10]

Yan-Ju Liu a,*, Yu-Xian Li a, Min Xu a, Xia Wang a
PMCID: PMC3050209  PMID: 21522551

Abstract

The crystal structure of the title compound, poly[bis­(tri­methyl­ammonium) hexa-μ1,1-azido-tetra­azido­tricobalt­ate(II,III)], [(CH3)3NH]2[CoIICoIII 2(N3)10], consists of anionic chains [CoIICoIII 2(N3)10]2− extending parallel to the c axis and [(CH3)3NH]+ counter-cations situated between the chains. In the anionic chain, one tetra­hedrally coordinated CoII atom (site symmetry 2) and two octa­hedrally coordinated CoIII atoms are arranged alternately and are linked by μ1,1-azide bridges. The anionic chains and cations are connected via N—H⋯N hydrogen bonding into a three-dimensional structure.

Related literature

For background to transition-metal azido-complexes templated by counter-cations of various sizes, see: Liu et al. (2006 ▶, 2008 ▶). For related cobalt complexes, see: Zhang et al. (2010 ▶).graphic file with name e-67-00m27-scheme1.jpg

Experimental

Crystal data

  • (C3H10N)2[Co3(N3)10]

  • M r = 717.33

  • Monoclinic, Inline graphic

  • a = 21.7200 (6) Å

  • b = 11.3812 (4) Å

  • c = 12.1628 (4) Å

  • β = 115.524 (2)°

  • V = 2713.21 (15) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.88 mm−1

  • T = 293 K

  • 0.10 × 0.06 × 0.05 mm

Data collection

  • Rigaku Saturn diffractometer

  • Absorption correction: multi-scan (REQAB; Jacobson, 1998 ▶) T min = 0.708, T max = 0.823

  • 22049 measured reflections

  • 2389 independent reflections

  • 1481 reflections with I > 2σ(I)

  • R int = 0.103

Refinement

  • R[F 2 > 2σ(F 2)] = 0.032

  • wR(F 2) = 0.061

  • S = 0.98

  • 2389 reflections

  • 190 parameters

  • 24 restraints

  • H-atom parameters constrained

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.35 e Å−3

Data collection: CrystalClear (Rigaku/MSC, 2006 ▶); 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: publCIF (Westrip, 2010 ▶).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810049421/wm2430sup1.cif

e-67-00m27-sup1.cif (20.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049421/wm2430Isup2.hkl

e-67-00m27-Isup2.hkl (117.5KB, hkl)

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

Table 1. Selected bond lengths (Å).

Co1—N7 1.944 (3)
Co1—N4 1.948 (3)
Co1—N10 1.964 (3)
Co1—N1 1.979 (3)
Co1—N13i 2.008 (3)
Co1—N13 2.008 (3)
Co2—N1ii 1.968 (3)
Co2—N1 1.968 (3)
Co2—N10i 2.014 (3)
Co2—N10iii 2.014 (3)

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

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N16—H16⋯N7 0.91 2.02 2.890 159

Acknowledgments

This study was supported by the Doctoral Research Fund of Henan Chinese Medicine (BSJJ2009–38).

supplementary crystallographic information

Comment

Azido-bridged complexes have attracted a lot of attention in recent times because of their importance in diverse fields, encompassing condensed matter physics, materials chemistry, biological chemistry, etc. Having diverse coordination modes and being an efficient magnetic coupler, the azide anion is a versatile ligand in bridging different transition metals, generating rich and fascinating architectures ranging from discrete polynuclears to extended three-dimensional networks with interesting magnetic properties (antiferromagnetic, ferromagnetic, ferrimagnetic, canted and alternating systems). In fact, remarkable structural variations of azido-bridged complexes have been reported by using various ancillary ligands, with different number of coordination sites and steric hindrance, to control over the dimensions of complexes and bridging modes of the azide anions, thus leading to the control over their magnetic properties. However, only a few metal-azido systems devoid of ancillary ligands have been obtained by varying the size of the coutercations (Liu et al., 2006, 2008). A small coutercation such as (CH3)4N+ produced the one-dimensional ferromagnetic complex [(CH3)4N][Cu(N3)3], in which the Cu(II) ions are connected by a triple azido-bridge, including two µ1,3-N3 and one µ1,1-N3 anions. When more bulky coutercations were employed, the mononuclear paramagnetic complex [(CH3CH2)4N]2[Cu(N3)4], the dinuclear antiferromagnetic complex [(CH3CH2CH2CH2)4N]2[Cu2(N3)6] and the one-dimensional ferromagnetic complex [(CH3CH2CH2)4N]2[Cu3(N3)8] were obtained separately. For magnese(II)-azido complexes, use of small coutercations like (CH3)4N+ and Cs+ produced compounds with interesting three-dimensional structures [(CH3)4N][Mn(N3)3] and Cs[Mn(N3)3], where the cations are situated in the voids the anionic MnII-azido network. When using the more bulky cation (CH3CH2)4N+, the one-dimensional ferromagnetic complex [(CH3CH2)4N][Mn(N3)3] was obtained. Despite the results obtained above, azido-bridged complexes with mixed-valent metal ions have not been reported. In this work, we report on a mixed-valence cobalt(II,III) complex, [(CH3)3NH]2[CoIICoIII2(N3)10], (I).

The structure of (I) consists of anionic chains [CoIICoIII2(N3)10]2- extending parallel to the c-axis. The [(CH3)3NH]+ countercations are situated between the chains (Fig. 1). In the [CoIICoIII2(N3)10]2- anionic chain, the CoII atom (Co2, site symmetry 2) is tetrahedrally coordinated by N atoms, whereas the CoIII atom (Co1) is octahedrally coordinated. CoII and CoIII atoms are linked by µ1,1-azido ligands and are alternatively arranged along the chain direction. The Co1—N distances range between 1.944 (3)–2.008 (3) Å, slightly longer than those expected for CoIII. The Co2—N distances range between 1.968 (3)–2.014 (3) Å, slightly shorter than those expected for CoII (Zhang et al., 2010). The anionic chain and the cations are connected via N—H···N hydrogen bonding between the donating N—H function of the cation and non-bridging azido groups of the anion (Fig 2).

Experimental

In a test tube a 5 ml methanol solution of 0.10M Co(ClO4)2.6H2O was layered carefully with 3 ml methanol and then with 10 ml methanol solution of 0.20M HCl, 0.20M NaN3, and 0.10M trimethylamine. The tube was sealed and kept undisturbed. Tiny red columnar crystals appeared overnight. Crystallization time of one week produced crystals in a yield of 25% based on the metal salt.

Refinement

Hydrogen atoms were added geometrically and were refined using a riding model, with C—H = 0.98 Å (CH3) and N—H = 0.89 Å.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title structure. All non-H atoms are labelled and are shown with displacement ellipsoids at the 30% probability level. H atoms have been omitted.

Fig. 2.

Fig. 2.

A view of the crystal packing along the c axis.

Crystal data

(C3H10N)2[Co3(N3)10] F(000) = 1444
Mr = 717.33 Dx = 1.756 Mg m−3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 14377 reflections
a = 21.7200 (6) Å θ = 3.4–25.0°
b = 11.3812 (4) Å µ = 1.88 mm−1
c = 12.1628 (4) Å T = 293 K
β = 115.524 (2)° Pillar, red
V = 2713.21 (15) Å3 0.10 × 0.06 × 0.05 mm
Z = 4

Data collection

Rigaku Saturn diffractometer 2389 independent reflections
Radiation source: fine-focus sealed tube 1481 reflections with I > 2σ(I)
graphite Rint = 0.103
Detector resolution: 0.76 pixels mm-1 θmax = 25.0°, θmin = 3.6°
dtprofit.ref scans h = −25→25
Absorption correction: multi-scan (REQAB; Jacobson, 1998) k = −13→13
Tmin = 0.708, Tmax = 0.823 l = −14→14
22049 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)] = 0.032 H-atom parameters constrained
wR(F2) = 0.061 w = 1/[σ2(Fo2) + (0.0204P)2] where P = (Fo2 + 2Fc2)/3
S = 0.98 (Δ/σ)max = 0.001
2389 reflections Δρmax = 0.31 e Å−3
190 parameters Δρmin = −0.35 e Å−3
24 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: 0.00084 (18)

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
Co1 0.04965 (2) 0.10300 (4) 0.05706 (4) 0.03529 (17)
Co2 0.0000 −0.04737 (5) 0.2500 0.0402 (2)
N1 0.06948 (14) 0.0409 (2) 0.2209 (3) 0.0428 (6)
N2 0.12002 (17) 0.0827 (3) 0.3042 (3) 0.0448 (6)
N3 0.16669 (18) 0.1210 (3) 0.3810 (3) 0.0740 (10)
N4 0.14720 (14) 0.1256 (2) 0.1097 (3) 0.0523 (7)
N5 0.16894 (15) 0.1348 (3) 0.0363 (3) 0.0540 (7)
N6 0.1925 (2) 0.1442 (4) −0.0308 (4) 0.1069 (15)
N7 0.04578 (16) 0.2621 (2) 0.1120 (3) 0.0489 (8)
N8 −0.00656 (18) 0.3009 (3) 0.1097 (3) 0.0504 (8)
N9 −0.05415 (18) 0.3426 (3) 0.1100 (3) 0.0806 (12)
N10 0.02748 (13) 0.1593 (3) −0.1084 (2) 0.0434 (6)
N11 0.04393 (15) 0.2609 (3) −0.1156 (2) 0.0492 (6)
N12 0.0599 (2) 0.3555 (3) −0.1195 (3) 0.0930 (13)
N13 −0.04827 (13) 0.0595 (2) 0.0083 (2) 0.0384 (6)
N14 −0.09288 (16) 0.1253 (3) −0.0627 (3) 0.0425 (6)
N15 −0.13450 (17) 0.1858 (3) −0.1255 (3) 0.0715 (10)
N16 0.16193 (14) 0.4179 (3) 0.2144 (3) 0.0539 (8)
H16 0.1336 0.3554 0.1828 0.065*
C1 0.2022 (2) 0.3949 (5) 0.3459 (4) 0.1044 (17)
H1A 0.2292 0.4628 0.3840 0.157*
H1B 0.2316 0.3287 0.3565 0.157*
H1C 0.1719 0.3783 0.3826 0.157*
C2 0.1190 (3) 0.5217 (4) 0.1950 (5) 0.1125 (19)
H2A 0.0852 0.5067 0.2242 0.169*
H2B 0.0970 0.5396 0.1096 0.169*
H2C 0.1468 0.5871 0.2384 0.169*
C3 0.2062 (2) 0.4251 (5) 0.1509 (4) 0.1121 (19)
H3A 0.1787 0.4379 0.0655 0.168*
H3B 0.2311 0.3529 0.1621 0.168*
H3C 0.2377 0.4891 0.1837 0.168*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Co1 0.0382 (3) 0.0364 (3) 0.0331 (3) −0.0041 (2) 0.0171 (2) −0.0013 (2)
Co2 0.0487 (4) 0.0370 (4) 0.0412 (5) 0.000 0.0253 (4) 0.000
N1 0.0456 (15) 0.0502 (15) 0.0338 (16) −0.0052 (12) 0.0181 (13) 0.0022 (12)
N2 0.0475 (15) 0.0518 (15) 0.0353 (16) −0.0042 (13) 0.0180 (13) 0.0033 (13)
N3 0.065 (2) 0.095 (3) 0.052 (2) −0.019 (2) 0.015 (2) −0.006 (2)
N4 0.0449 (15) 0.0647 (16) 0.0528 (17) −0.0104 (12) 0.0264 (12) −0.0027 (13)
N5 0.0453 (15) 0.0637 (16) 0.0561 (18) −0.0079 (12) 0.0249 (13) −0.0055 (13)
N6 0.097 (3) 0.148 (4) 0.112 (4) −0.027 (3) 0.079 (3) −0.026 (3)
N7 0.061 (2) 0.0407 (19) 0.051 (2) −0.0085 (16) 0.0293 (18) −0.0088 (15)
N8 0.062 (2) 0.040 (2) 0.050 (2) −0.0019 (17) 0.025 (2) −0.0050 (15)
N9 0.071 (3) 0.068 (3) 0.103 (3) 0.009 (2) 0.037 (3) −0.020 (2)
N10 0.0570 (15) 0.0435 (16) 0.0329 (14) −0.0095 (13) 0.0222 (12) 0.0004 (13)
N11 0.0626 (15) 0.0478 (16) 0.0348 (15) −0.0086 (14) 0.0186 (12) 0.0007 (13)
N12 0.150 (4) 0.054 (2) 0.064 (3) −0.036 (2) 0.036 (3) 0.004 (2)
N13 0.0378 (15) 0.0388 (15) 0.0414 (17) −0.0002 (10) 0.0197 (13) −0.0025 (11)
N14 0.0408 (15) 0.0412 (16) 0.0447 (17) −0.0017 (11) 0.0176 (13) −0.0036 (11)
N15 0.058 (2) 0.058 (2) 0.081 (3) 0.0085 (19) 0.014 (2) 0.005 (2)
N16 0.0501 (19) 0.050 (2) 0.061 (2) −0.0163 (15) 0.0234 (19) −0.0118 (16)
C1 0.083 (3) 0.143 (5) 0.067 (4) −0.039 (3) 0.013 (3) 0.007 (3)
C2 0.115 (4) 0.052 (3) 0.165 (6) 0.015 (3) 0.055 (4) −0.001 (3)
C3 0.093 (4) 0.173 (5) 0.099 (4) −0.055 (4) 0.069 (3) −0.045 (4)

Geometric parameters (Å, °)

Co1—N7 1.944 (3) N11—N12 1.139 (4)
Co1—N4 1.948 (3) N13—N14 1.234 (4)
Co1—N10 1.964 (3) N13—Co1i 2.008 (3)
Co1—N1 1.979 (3) N14—N15 1.131 (4)
Co1—N13i 2.008 (3) N16—C2 1.460 (5)
Co1—N13 2.008 (3) N16—C3 1.473 (4)
Co2—N1ii 1.968 (3) N16—C1 1.478 (5)
Co2—N1 1.968 (3) N16—H16 0.9100
Co2—N10i 2.014 (3) C1—H1A 0.9600
Co2—N10iii 2.014 (3) C1—H1B 0.9600
N1—N2 1.224 (4) C1—H1C 0.9600
N2—N3 1.129 (4) C2—H2A 0.9600
N4—N5 1.181 (4) C2—H2B 0.9600
N5—N6 1.140 (4) C2—H2C 0.9600
N7—N8 1.209 (4) C3—H3A 0.9600
N8—N9 1.139 (4) C3—H3B 0.9600
N10—N11 1.225 (4) C3—H3C 0.9600
N10—Co2i 2.014 (3)
N7—Co1—N4 88.05 (12) Co1—N10—Co2i 121.43 (14)
N7—Co1—N10 91.18 (12) N12—N11—N10 178.5 (4)
N4—Co1—N10 92.62 (12) N14—N13—Co1i 114.1 (2)
N7—Co1—N1 90.55 (12) N14—N13—Co1 118.0 (2)
N4—Co1—N1 88.97 (12) Co1i—N13—Co1 100.22 (11)
N10—Co1—N1 177.69 (12) N15—N14—N13 178.2 (4)
N7—Co1—N13i 176.56 (13) C2—N16—C3 112.7 (4)
N4—Co1—N13i 94.61 (11) C2—N16—C1 110.9 (4)
N10—Co1—N13i 86.53 (11) C3—N16—C1 111.2 (3)
N1—Co1—N13i 91.67 (11) C2—N16—H16 107.3
N7—Co1—N13 97.71 (11) C3—N16—H16 107.3
N4—Co1—N13 173.16 (12) C1—N16—H16 107.3
N10—Co1—N13 90.96 (11) N16—C1—H1A 109.5
N1—Co1—N13 87.29 (11) N16—C1—H1B 109.5
N13i—Co1—N13 79.78 (11) H1A—C1—H1B 109.5
N1ii—Co2—N1 118.61 (16) N16—C1—H1C 109.5
N1ii—Co2—N10i 120.58 (11) H1A—C1—H1C 109.5
N1—Co2—N10i 97.86 (11) H1B—C1—H1C 109.5
N1ii—Co2—N10iii 97.86 (11) N16—C2—H2A 109.5
N1—Co2—N10iii 120.58 (11) N16—C2—H2B 109.5
N10i—Co2—N10iii 101.58 (16) H2A—C2—H2B 109.5
N2—N1—Co2 122.3 (2) N16—C2—H2C 109.5
N2—N1—Co1 115.0 (2) H2A—C2—H2C 109.5
Co2—N1—Co1 120.82 (15) H2B—C2—H2C 109.5
N3—N2—N1 179.9 (5) N16—C3—H3A 109.5
N5—N4—Co1 119.7 (3) N16—C3—H3B 109.5
N6—N5—N4 177.2 (4) H3A—C3—H3B 109.5
N8—N7—Co1 120.8 (2) N16—C3—H3C 109.5
N9—N8—N7 176.5 (4) H3A—C3—H3C 109.5
N11—N10—Co1 115.5 (2) H3B—C3—H3C 109.5
N11—N10—Co2i 121.6 (2)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N16—H16···N7 0.91 2.02 2.890 159.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2430).

References

  1. Jacobson, R. (1998). REQAB Private communication to the Rigaku Corporation, Tokyo, Japan.
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  4. Rigaku/MSC (2006). CrystalClear Rigaku/MSC, The Woodlands, Texas, USA.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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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 I, global. DOI: 10.1107/S1600536810049421/wm2430sup1.cif

e-67-00m27-sup1.cif (20.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049421/wm2430Isup2.hkl

e-67-00m27-Isup2.hkl (117.5KB, hkl)

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


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