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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jun 5;66(Pt 7):m743. doi: 10.1107/S1600536810020714

Bis{4,4′-[oxalylbis(aza­nedi­yl)]dipyridinium} octa­molybdate

Jianbo Qin a, Jingren Dong a, Jinghua Li b, Yun Gong a,*
PMCID: PMC3006793  PMID: 21587682

Abstract

In the crystal structure of the title compound, (C12H12N4O2)2[Mo8O26], the amino and pyridinium groups of the N 1,N 2-di(pyridinium-4-yl)oxalamide cations are hydrogen bonded to the O atoms of the centrosymmetric isopolyoxometalate β-[Mo8O26]4− anions, forming a three-dimensional supra­molecular architecture.

Related literature

For polyoxometalates (POMs), see: Cronin et al. (2002); Fukaya & Yamase (2003); Katsoulis (1988); Pope & Müller (1991). For the applications of POMs in biology and materials sciences, see: Cui et al. (2003); Luan et al. (2002); Wang et al. (2003). For the structure of N 1,N 2-di(pyridin-4-yl)oxalamide, see: Tzeng et al. (2007). For details of the geometrical parameters in the same isopolyoxometalate anion, see: Gong et al. (2007).graphic file with name e-66-0m743-scheme1.jpg

Experimental

Crystal data

  • (C12H12N4O2)2[Mo8O26]

  • M r = 1672.03

  • Monoclinic, Inline graphic

  • a = 10.633 (2) Å

  • b = 11.552 (2) Å

  • c = 17.240 (4) Å

  • β = 101.553 (3)°

  • V = 2074.7 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.45 mm−1

  • T = 293 K

  • 0.23 × 0.22 × 0.05 mm

Data collection

  • Siemens SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.829, T max = 1.000

  • 14669 measured reflections

  • 4534 independent reflections

  • 4215 reflections with I > 2σ(I)

  • R int = 0.021

Refinement

  • R[F 2 > 2σ(F 2)] = 0.022

  • wR(F 2) = 0.098

  • S = 1.40

  • 4534 reflections

  • 316 parameters

  • H-atom parameters constrained

  • Δρmax = 1.40 e Å−3

  • Δρmin = −2.27 e Å−3

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1996); 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 datablocks global, I. DOI: 10.1107/S1600536810020714/su2182sup1.cif

e-66-0m743-sup1.cif (21.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810020714/su2182Isup2.hkl

e-66-0m743-Isup2.hkl (222.1KB, 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
N2—H2A⋯O7i 0.86 2.61 3.368 (4) 148
N1—H1⋯O8ii 0.86 1.89 2.699 (4) 158
N3—H3⋯O5iii 0.86 1.94 2.779 (4) 165
N4—H4A⋯O1 0.86 2.25 2.669 (4) 110
N4—H4A⋯O4iv 0.86 2.26 3.059 (4) 154

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

Acknowledgments

This work was supported by the Chongqing University Postgraduate Science Fund (No. 200911A1B0010317) and the Fundamental Research Funds for the Central Universities (No. CDJZR10 22 00 09)

supplementary crystallographic information

Comment

Polyoxometalates (POMs) are early transition metal oxygen anion clusters. They are an outstanding class of anionic compounds due to their wealthy topology, superior physical and chemical properties (Pope & Muller, 1991; Katsoulis, 1988). The nanoscopic sizes (Cronin, et al., 2002; Fukaya & Yamase, 2003,) and thier diversified shapes of discrete POMs have attracted great interest. The design, synthesis and structural characterization of inorganic-organic hybrid compounds base on POMs, for which many properties and applications can be predicted, have established a new field of research in the chemistry of biology and materials sciences (Luan, et al., 2002; Cui, et al., 2003; Wang, et al., 2003). Different N-heterocycle ligands can lead to different inorganic-organic hybrid compounds based on POMs. N1,N2-di(pyridin-4-yl)oxalamide (L), is a bis-pyridine ligand, which has been reported only rarely in the construction of hybrid compounds based on POMs. In the present work, the title complex was synthesized hydrothermally by reacting L with the isopolyoxometalate, Mo8O26.

The molecular structure of the title complex is illustrated in Fig. 1. In the asymmetric unit there is a doublely protonated L molecule, and half an isopolyoxometalate unit. The bond distances and angles in the cation are similar to those observed previously for N1,N2-di(pyridin-4-yl)oxalamide (Tzeng, et al., 2007). For the anion, [Mo8O26]4-, the geometrical parameters are similar to those reported by (Gong, et al., 2007).

In the crystal the protonated pyrdidinium groups and the amino group form N-H···O hydrogen bonds with the oxygen atoms of the centrosymmetric [Mo8O26]4- anions, leading to the formation of a three dimensional supramolecular network (Table 1 and Fig. 2).

Experimental

A mixture of L (0.05 mmol, 0.012 g), Na2MoO4(0.05 mmol, 0.012 g) and water(10 ml) was adjusted to pH = 3.0 by HCl. The synthesis was carried out hydrothermally using a Teflon-lined autoclave. The reaction mixture was heated at 393 K for 3 days, followed by slow cooling to rt. The resulting colorless prismatic crystals were filtered off and washed with water (yield: ca. 90% based on Mo). Elemental analyse - found: C, 17.45; H, 1.58; N, 6.56; Mo, 46.11; calcd: C, 17.22; H, 1.44; N, 6.70; Mo, 45.93.

Refinement

The H-atoms were positioned geometrically and refined as riding atoms: C—H = 0.93Å, N—H = 0.86Å and Uiso(H) = 1.2Ueq(N,C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title complex, with the atomic numbering scheme and displacement ellipsoids at the 30% probability level [Symmetry codes: (i) -x,-y+1,-z].

Fig. 2.

Fig. 2.

A view along the b-axis of the crystal packing of the title complex, illustrating the three dimensional supramolecular architecture constructed by the intermolecular N-H···O hydrogen bonds (dotted lines); see Table 1 for details.

Crystal data

(C12H12N4O2)2[Mo8O26] F(000) = 1592
Mr = 1672.03 Dx = 2.670 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 5569 reflections
a = 10.633 (2) Å θ = 2.1–27.5°
b = 11.552 (2) Å µ = 2.45 mm1
c = 17.240 (4) Å T = 293 K
β = 101.553 (3)° Prism, colorless
V = 2074.7 (8) Å3 0.23 × 0.22 × 0.05 mm
Z = 2

Data collection

Siemens CCD area-detector diffractometer 4534 independent reflections
Radiation source: fine-focus sealed tube 4215 reflections with I > 2σ(I)
graphite Rint = 0.021
φ and ω scans θmax = 27.5°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −13→13
Tmin = 0.829, Tmax = 1.000 k = −13→14
14669 measured reflections l = −22→17

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)] = 0.022 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.098 H-atom parameters constrained
S = 1.40 w = 1/[σ2(Fo2) + (0.054P)2 + 0.4946P] where P = (Fo2 + 2Fc2)/3
4534 reflections (Δ/σ)max = 0.001
316 parameters Δρmax = 1.40 e Å3
0 restraints Δρmin = −2.27 e Å3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
Mo1 0.08119 (2) 0.53770 (2) 0.098624 (15) 0.01481 (10)
Mo2 0.03951 (3) 0.71904 (2) −0.069243 (16) 0.01713 (10)
Mo3 0.25513 (2) 0.49409 (2) −0.029720 (16) 0.01602 (10)
Mo4 −0.13294 (3) 0.77083 (2) 0.064661 (17) 0.01917 (10)
O12 0.0104 (2) 0.8099 (2) 0.01704 (14) 0.0218 (5)
O6 0.2011 (2) 0.4893 (2) 0.17096 (15) 0.0252 (5)
O15 0.1779 (2) 0.61483 (18) 0.02814 (13) 0.0168 (4)
O5 −0.0636 (2) 0.44017 (19) 0.11312 (13) 0.0165 (4)
O4 −0.2513 (2) 0.8238 (2) −0.00841 (16) 0.0297 (6)
O7 0.3709 (2) 0.4459 (2) 0.04628 (15) 0.0275 (5)
N2 0.5229 (3) 0.1925 (2) 1.09498 (17) 0.0221 (6)
H2A 0.5102 0.2587 1.0720 0.026*
O13 0.0261 (2) 0.6628 (2) 0.13799 (13) 0.0205 (5)
C2 0.3935 (3) 0.2606 (3) 1.1832 (2) 0.0259 (7)
H2 0.3675 0.3224 1.1491 0.031*
O11 0.3343 (2) 0.5745 (2) −0.08718 (14) 0.0242 (5)
O9 −0.0852 (3) 0.7563 (2) −0.14308 (15) 0.0274 (5)
O10 0.1691 (3) 0.7832 (2) −0.09476 (16) 0.0273 (5)
C5 0.4718 (4) 0.0833 (3) 1.2863 (2) 0.0301 (8)
H5 0.4985 0.0245 1.3227 0.036*
C4 0.5210 (4) 0.0892 (3) 1.2190 (2) 0.0265 (7)
H4 0.5801 0.0346 1.2091 0.032*
N1 0.3858 (3) 0.1609 (3) 1.30054 (17) 0.0280 (7)
H1 0.3545 0.1541 1.3426 0.034*
O3 −0.1253 (3) 0.8654 (2) 0.14042 (16) 0.0321 (6)
C3 0.4805 (3) 0.1793 (3) 1.16520 (18) 0.0196 (6)
C1 0.3471 (4) 0.2490 (3) 1.2508 (2) 0.0286 (8)
H1A 0.2882 0.3025 1.2626 0.034*
O14 0.0844 (2) 0.40727 (19) 0.01120 (12) 0.0173 (4)
O8 0.2273 (2) 0.3590 (2) −0.09586 (13) 0.0205 (5)
N3 0.8440 (3) 0.0969 (3) 0.75088 (17) 0.0285 (7)
H3 0.8761 0.0988 0.7089 0.034*
O2 0.5624 (3) 0.2419 (2) 0.94778 (15) 0.0289 (6)
O1 0.6119 (3) 0.0145 (2) 1.08260 (16) 0.0334 (6)
N4 0.6865 (3) 0.0776 (3) 0.94989 (17) 0.0236 (6)
H4A 0.7065 0.0154 0.9770 0.028*
C11 0.7132 (3) 0.1824 (3) 0.8303 (2) 0.0261 (7)
H11 0.6606 0.2428 0.8399 0.031*
C10 0.7680 (4) 0.1841 (3) 0.7648 (2) 0.0298 (8)
H10 0.7525 0.2461 0.7297 0.036*
C8 0.8193 (4) 0.0012 (3) 0.8668 (2) 0.0303 (8)
H8 0.8384 −0.0609 0.9015 0.036*
C9 0.8712 (4) 0.0072 (3) 0.8005 (2) 0.0333 (9)
H9 0.9256 −0.0512 0.7898 0.040*
C12 0.7373 (3) 0.0892 (3) 0.88212 (18) 0.0204 (6)
C6 0.5830 (3) 0.1107 (3) 1.05882 (19) 0.0206 (6)
C7 0.6084 (3) 0.1539 (3) 0.97837 (19) 0.0226 (7)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Mo1 0.01333 (15) 0.02061 (16) 0.01084 (15) −0.00116 (9) 0.00325 (10) −0.00091 (10)
Mo2 0.01807 (16) 0.01867 (16) 0.01602 (16) 0.00122 (10) 0.00673 (11) 0.00088 (10)
Mo3 0.01266 (15) 0.02166 (17) 0.01468 (16) 0.00069 (9) 0.00496 (11) 0.00006 (10)
Mo4 0.01891 (17) 0.02088 (16) 0.01936 (16) 0.00103 (10) 0.00773 (12) −0.00038 (10)
O12 0.0232 (12) 0.0214 (11) 0.0228 (11) −0.0027 (9) 0.0093 (10) −0.0038 (9)
O6 0.0216 (12) 0.0342 (13) 0.0184 (12) 0.0020 (10) 0.0003 (10) 0.0029 (10)
O15 0.0156 (10) 0.0194 (10) 0.0160 (10) −0.0018 (8) 0.0047 (8) −0.0007 (9)
O5 0.0162 (10) 0.0199 (10) 0.0146 (10) 0.0006 (8) 0.0057 (8) 0.0005 (9)
O4 0.0250 (13) 0.0339 (14) 0.0311 (14) 0.0052 (11) 0.0073 (11) 0.0089 (11)
O7 0.0216 (12) 0.0381 (14) 0.0221 (12) 0.0048 (11) 0.0026 (10) 0.0052 (11)
N2 0.0260 (15) 0.0251 (14) 0.0176 (13) 0.0021 (12) 0.0105 (11) 0.0042 (11)
O13 0.0204 (11) 0.0226 (11) 0.0192 (11) −0.0004 (9) 0.0059 (9) −0.0040 (9)
C2 0.0268 (18) 0.0300 (17) 0.0226 (17) 0.0055 (14) 0.0089 (14) 0.0044 (14)
O11 0.0217 (12) 0.0292 (12) 0.0237 (12) −0.0022 (10) 0.0091 (10) 0.0032 (10)
O9 0.0291 (13) 0.0281 (12) 0.0232 (12) 0.0072 (11) 0.0010 (11) 0.0008 (11)
O10 0.0272 (13) 0.0269 (13) 0.0305 (13) −0.0026 (10) 0.0127 (11) 0.0019 (10)
C5 0.038 (2) 0.0303 (18) 0.0222 (17) 0.0010 (16) 0.0069 (15) 0.0068 (15)
C4 0.0269 (18) 0.0316 (18) 0.0222 (17) 0.0038 (14) 0.0074 (14) 0.0026 (15)
N1 0.0295 (16) 0.0401 (17) 0.0171 (13) −0.0029 (13) 0.0114 (12) −0.0004 (13)
O3 0.0354 (14) 0.0310 (13) 0.0332 (14) 0.0015 (11) 0.0146 (12) −0.0097 (12)
C3 0.0180 (15) 0.0268 (16) 0.0148 (14) −0.0016 (12) 0.0053 (12) 0.0005 (13)
C1 0.0263 (18) 0.0380 (19) 0.0235 (17) 0.0048 (15) 0.0097 (15) −0.0007 (16)
O14 0.0169 (10) 0.0209 (10) 0.0153 (10) 0.0003 (8) 0.0063 (8) 0.0001 (9)
O8 0.0223 (11) 0.0228 (11) 0.0193 (11) 0.0002 (9) 0.0110 (9) −0.0029 (9)
N3 0.0311 (16) 0.0405 (17) 0.0173 (13) −0.0040 (14) 0.0130 (12) −0.0015 (13)
O2 0.0333 (14) 0.0309 (13) 0.0244 (13) 0.0054 (11) 0.0104 (11) 0.0031 (11)
O1 0.0461 (17) 0.0300 (14) 0.0293 (14) 0.0072 (12) 0.0204 (13) 0.0039 (11)
N4 0.0278 (15) 0.0276 (14) 0.0188 (13) 0.0042 (12) 0.0127 (12) 0.0029 (12)
C11 0.0261 (17) 0.0322 (18) 0.0218 (16) 0.0051 (14) 0.0090 (14) 0.0019 (14)
C10 0.0299 (19) 0.040 (2) 0.0209 (17) 0.0027 (16) 0.0074 (15) 0.0061 (15)
C8 0.040 (2) 0.0269 (18) 0.0284 (19) 0.0052 (15) 0.0175 (17) 0.0041 (15)
C9 0.042 (2) 0.0317 (19) 0.032 (2) −0.0007 (16) 0.0210 (18) −0.0033 (16)
C12 0.0232 (16) 0.0244 (16) 0.0155 (14) −0.0036 (13) 0.0081 (12) −0.0026 (12)
C6 0.0195 (15) 0.0278 (16) 0.0171 (14) −0.0042 (13) 0.0094 (12) −0.0017 (13)
C7 0.0235 (16) 0.0286 (16) 0.0172 (15) −0.0049 (14) 0.0076 (13) −0.0018 (14)

Geometric parameters (Å, °)

Mo1—O6 1.690 (2) C2—C3 1.395 (5)
Mo1—O13 1.747 (2) C2—H2 0.9300
Mo1—O15 1.956 (2) C5—N1 1.338 (5)
Mo1—O5 1.964 (2) C5—C4 1.366 (5)
Mo1—O14 2.136 (2) C5—H5 0.9300
Mo1—O14i 2.399 (2) C4—C3 1.403 (5)
Mo1—Mo3 3.1951 (6) C4—H4 0.9300
Mo2—O10 1.699 (3) N1—C1 1.342 (5)
Mo2—O9 1.699 (3) N1—H1 0.8600
Mo2—O12 1.896 (2) C1—H1A 0.9300
Mo2—O5i 2.024 (2) O14—Mo2i 2.322 (2)
Mo2—O14i 2.322 (2) O14—Mo1i 2.399 (2)
Mo2—O15 2.333 (2) O8—Mo4i 1.939 (2)
Mo3—O11 1.699 (2) N3—C9 1.338 (5)
Mo3—O7 1.702 (2) N3—C10 1.342 (5)
Mo3—O8 1.921 (2) N3—H3 0.8600
Mo3—O15 1.986 (2) O2—C7 1.203 (4)
Mo3—O14 2.305 (2) O1—C6 1.203 (4)
Mo3—O5i 2.370 (2) N4—C7 1.368 (4)
Mo4—O3 1.692 (3) N4—C12 1.388 (4)
Mo4—O4 1.706 (3) N4—H4A 0.8600
Mo4—O12 1.924 (2) C11—C10 1.371 (5)
Mo4—O8i 1.939 (2) C11—C12 1.390 (5)
Mo4—O13 2.271 (2) C11—H11 0.9300
O5—Mo2i 2.024 (2) C10—H10 0.9300
O5—Mo3i 2.370 (2) C8—C9 1.368 (5)
N2—C6 1.360 (4) C8—C12 1.398 (5)
N2—C3 1.383 (4) C8—H8 0.9300
N2—H2A 0.8600 C9—H9 0.9300
C2—C1 1.361 (5) C6—C7 1.548 (5)
O6—Mo1—O13 104.42 (12) O12—Mo4—O13 78.54 (10)
O6—Mo1—O15 101.34 (11) O8i—Mo4—O13 77.86 (9)
O13—Mo1—O15 97.08 (10) Mo2—O12—Mo4 118.21 (12)
O6—Mo1—O5 102.18 (11) Mo1—O15—Mo3 108.29 (10)
O13—Mo1—O5 95.32 (10) Mo1—O15—Mo2 110.37 (10)
O15—Mo1—O5 149.67 (9) Mo3—O15—Mo2 105.41 (9)
O6—Mo1—O14 99.85 (11) Mo1—O5—Mo2i 108.21 (10)
O13—Mo1—O14 155.72 (10) Mo1—O5—Mo3i 109.83 (10)
O15—Mo1—O14 78.37 (9) Mo2i—O5—Mo3i 102.84 (9)
O5—Mo1—O14 78.98 (9) C6—N2—C3 126.2 (3)
O6—Mo1—O14i 174.94 (10) C6—N2—H2A 116.9
O13—Mo1—O14i 80.62 (9) C3—N2—H2A 116.9
O15—Mo1—O14i 77.46 (8) Mo1—O13—Mo4 120.57 (11)
O5—Mo1—O14i 77.42 (8) C1—C2—C3 119.6 (3)
O14—Mo1—O14i 75.11 (9) C1—C2—H2 120.2
O6—Mo1—Mo3 90.19 (9) C3—C2—H2 120.2
O13—Mo1—Mo3 133.25 (8) N1—C5—C4 121.0 (3)
O15—Mo1—Mo3 36.17 (6) N1—C5—H5 119.5
O5—Mo1—Mo3 125.10 (6) C4—C5—H5 119.5
O14—Mo1—Mo3 46.13 (6) C5—C4—C3 118.6 (3)
O14i—Mo1—Mo3 86.01 (5) C5—C4—H4 120.7
O10—Mo2—O9 104.31 (13) C3—C4—H4 120.7
O10—Mo2—O12 103.29 (11) C5—N1—C1 121.6 (3)
O9—Mo2—O12 102.84 (11) C5—N1—H1 119.2
O10—Mo2—O5i 97.46 (11) C1—N1—H1 119.2
O9—Mo2—O5i 95.06 (11) N2—C3—C2 117.9 (3)
O12—Mo2—O5i 148.09 (10) N2—C3—C4 123.3 (3)
O10—Mo2—O14i 160.99 (11) C2—C3—C4 118.8 (3)
O9—Mo2—O14i 93.28 (11) N1—C1—C2 120.3 (3)
O12—Mo2—O14i 79.28 (9) N1—C1—H1A 119.8
O5i—Mo2—O14i 73.47 (8) C2—C1—H1A 119.8
O10—Mo2—O15 89.10 (11) Mo1—O14—Mo3 91.94 (8)
O9—Mo2—O15 162.69 (11) Mo1—O14—Mo2i 92.79 (8)
O12—Mo2—O15 84.24 (9) Mo3—O14—Mo2i 162.71 (11)
O5i—Mo2—O15 72.02 (8) Mo1—O14—Mo1i 104.89 (9)
O14i—Mo2—O15 72.31 (8) Mo3—O14—Mo1i 98.15 (8)
O11—Mo3—O7 105.16 (12) Mo2i—O14—Mo1i 96.69 (8)
O11—Mo3—O8 97.69 (11) Mo3—O8—Mo4i 119.38 (11)
O7—Mo3—O8 101.11 (12) C9—N3—C10 121.9 (3)
O11—Mo3—O15 102.23 (11) C9—N3—H3 119.1
O7—Mo3—O15 98.71 (11) C10—N3—H3 119.1
O8—Mo3—O15 147.03 (9) C7—N4—C12 127.3 (3)
O11—Mo3—O14 158.28 (10) C7—N4—H4A 116.3
O7—Mo3—O14 96.57 (11) C12—N4—H4A 116.3
O8—Mo3—O14 77.93 (9) C10—C11—C12 119.1 (3)
O15—Mo3—O14 73.83 (8) C10—C11—H11 120.4
O11—Mo3—O5i 86.39 (10) C12—C11—H11 120.4
O7—Mo3—O5i 166.64 (10) N3—C10—C11 120.4 (3)
O8—Mo3—O5i 83.62 (9) N3—C10—H10 119.8
O15—Mo3—O5i 71.82 (8) C11—C10—H10 119.8
O14—Mo3—O5i 72.03 (8) C9—C8—C12 119.5 (3)
O11—Mo3—Mo1 137.78 (9) C9—C8—H8 120.3
O7—Mo3—Mo1 87.02 (9) C12—C8—H8 120.3
O8—Mo3—Mo1 119.84 (7) N3—C9—C8 120.1 (4)
O15—Mo3—Mo1 35.55 (6) N3—C9—H9 119.9
O14—Mo3—Mo1 41.93 (5) C8—C9—H9 119.9
O5i—Mo3—Mo1 79.83 (5) N4—C12—C11 124.3 (3)
O3—Mo4—O4 104.63 (14) N4—C12—C8 116.8 (3)
O3—Mo4—O12 104.98 (12) C11—C12—C8 118.9 (3)
O4—Mo4—O12 97.54 (12) O1—C6—N2 126.7 (3)
O3—Mo4—O8i 103.44 (11) O1—C6—C7 121.6 (3)
O4—Mo4—O8i 97.81 (12) N2—C6—C7 111.6 (3)
O12—Mo4—O8i 142.92 (9) O2—C7—N4 127.6 (3)
O3—Mo4—O13 90.56 (11) O2—C7—C6 122.5 (3)
O4—Mo4—O13 164.80 (11) N4—C7—C6 110.0 (3)

Symmetry codes: (i) −x, −y+1, −z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H2A···O7ii 0.86 2.61 3.368 (4) 148
N1—H1···O8iii 0.86 1.89 2.699 (4) 158
N3—H3···O5iv 0.86 1.94 2.779 (4) 165
N4—H4A···O1 0.86 2.25 2.669 (4) 110
N4—H4A···O4v 0.86 2.26 3.059 (4) 154

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2182).

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/S1600536810020714/su2182sup1.cif

e-66-0m743-sup1.cif (21.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810020714/su2182Isup2.hkl

e-66-0m743-Isup2.hkl (222.1KB, hkl)

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


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