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The structure of poly[[(ethylenediamine-
2N,N')cobalt(II)]-
-tetraoxomolybdato(VI)], [Co(C
2H
8N
2)MoO
4]
n or [CoMoO
4(C
2H
8N
2)]
n, is composed of puckered layers constructed from MoO
4 tetrahedra and CoN
2O
4 octahedra, with the ethylenediamine ligand coordinated to the Co atom in a
cis fashion. Each pair of cobalt sites forms a binuclear edge-sharing unit through a {Co
2O
2} interaction. The binuclear octahedral units are interconnected through the bridging MoO
4 tetrahedra into a layer structure.
Supporting information
CCDC reference: 184480
Data collection: MSC/AFC Diffractometer Control Software
(Molecular Structure Corporation, 1987); cell refinement: TEXSAN (Molecular Structure Corporation, 1987); data reduction: TEXRAY in TEXSAN; program(s) used to solve structure: SHELXS86 (Sheldrick, 1990a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL/PC (Sheldrick, 1990b); software used to prepare material for publication: SHELXL97.
Polymeric [ethylenediamine-cobalt(II)] molybdate(VI)
top
Crystal data top
C2H8CoMoN2O4 | F(000) = 540 |
Mr = 278.97 | Dx = 2.670 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71069 Å |
Hall symbol: -P 2ybc | Cell parameters from 300 reflections |
a = 10.3955 (6) Å | θ = 10–25° |
b = 9.7127 (8) Å | µ = 4.15 mm−1 |
c = 7.1234 (4) Å | T = 293 K |
β = 105.236 (6)° | Plate, violet |
V = 693.96 (8) Å3 | 0.12 × 0.10 × 0.08 mm |
Z = 4 | |
Data collection top
Rigaku AFC-5R diffractometer | 1461 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.038 |
Graphite monochromator | θmax = 27.5°, θmin = 2.9° |
ω–2θ scans | h = −13→13 |
Absorption correction: ψ scan (North et al., 1968) | k = −12→0 |
Tmin = 0.614, Tmax = 0.716 | l = 0→9 |
6370 measured reflections | 3 standard reflections every 150 reflections |
1590 independent reflections | intensity decay: 0.2% |
Refinement top
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: difference Fourier map |
wR(F2) = 0.054 | H-atom parameters not refined |
S = 1.02 | w = 1/[σ2(Fo2) + (0.0304P)2] where P = (Fo2 + 2Fc2)/3 |
1590 reflections | (Δ/σ)max = 0.002 |
91 parameters | Δρmax = 0.82 e Å−3 |
0 restraints | Δρmin = −0.67 e Å−3 |
Special details top
Experimental. crystal coated in epoxy glue |
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) top | x | y | z | Uiso*/Ueq | |
Mo | 0.34406 (2) | 0.395709 (19) | 0.29607 (3) | 0.01601 (8) | |
Co | 0.37886 (3) | 0.02788 (3) | 0.31572 (4) | 0.01677 (10) | |
O1 | 0.42317 (19) | 0.23468 (17) | 0.3482 (3) | 0.0234 (4) | |
O2 | 0.1778 (2) | 0.3679 (2) | 0.1793 (3) | 0.0316 (4) | |
O3 | 0.3554 (2) | 0.48648 (19) | 0.5138 (2) | 0.0280 (4) | |
O4 | 0.41481 (18) | 0.48974 (17) | 0.1294 (2) | 0.0192 (4) | |
N1 | 0.3273 (2) | −0.1844 (2) | 0.3113 (3) | 0.0238 (4) | |
H1A | 0.3388 | −0.2254 | 0.2029 | 0.080* | |
H1B | 0.3796 | −0.2283 | 0.4154 | 0.080* | |
N2 | 0.1685 (2) | 0.0530 (2) | 0.2656 (3) | 0.0236 (4) | |
H2A | 0.1461 | 0.1232 | 0.1812 | 0.050* | |
H2B | 0.1591 | 0.0827 | 0.3790 | 0.050* | |
C1 | 0.1865 (3) | −0.1933 (3) | 0.3148 (4) | 0.0306 (6) | |
H1C | 0.1866 | −0.1786 | 0.4447 | 0.050* | |
H1D | 0.1499 | −0.2762 | 0.2692 | 0.050* | |
C2 | 0.1064 (3) | −0.0794 (3) | 0.1919 (4) | 0.0284 (6) | |
H2C | 0.1066 | −0.0911 | 0.0582 | 0.050* | |
H2D | 0.0158 | −0.0817 | 0.2003 | 0.050* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Mo | 0.01930 (13) | 0.01660 (12) | 0.01333 (12) | 0.00156 (7) | 0.00642 (8) | 0.00213 (6) |
Co | 0.01892 (18) | 0.01729 (16) | 0.01453 (16) | −0.00028 (13) | 0.00513 (13) | −0.00016 (11) |
O1 | 0.0290 (10) | 0.0171 (8) | 0.0241 (8) | 0.0004 (8) | 0.0067 (7) | 0.0011 (7) |
O2 | 0.0234 (10) | 0.0424 (11) | 0.0279 (10) | −0.0030 (9) | 0.0048 (8) | 0.0071 (9) |
O3 | 0.0402 (12) | 0.0291 (9) | 0.0178 (8) | 0.0064 (9) | 0.0134 (8) | 0.0005 (7) |
O4 | 0.0226 (9) | 0.0201 (8) | 0.0160 (8) | −0.0023 (7) | 0.0071 (7) | 0.0004 (6) |
N1 | 0.0294 (12) | 0.0212 (9) | 0.0210 (10) | −0.0010 (10) | 0.0069 (9) | 0.0002 (8) |
N2 | 0.0231 (11) | 0.0263 (11) | 0.0209 (10) | 0.0033 (10) | 0.0050 (8) | −0.0005 (9) |
C1 | 0.0336 (15) | 0.0289 (13) | 0.0308 (14) | −0.0062 (13) | 0.0114 (12) | 0.0039 (11) |
C2 | 0.0213 (13) | 0.0342 (13) | 0.0284 (13) | −0.0031 (12) | 0.0040 (10) | 0.0001 (11) |
Geometric parameters (Å, º) top
Mo—O2 | 1.731 (2) | N1—H1A | 0.90 |
Mo—O1 | 1.7607 (17) | N1—H1B | 0.90 |
Mo—O3 | 1.7606 (17) | N2—C2 | 1.472 (3) |
Mo—O4 | 1.8007 (16) | N2—H2A | 0.90 |
Co—O1 | 2.0601 (17) | N2—H2B | 0.89 |
Co—O3i | 2.1048 (17) | C1—C2 | 1.517 (4) |
Co—O4ii | 2.1095 (18) | C1—H1C | 0.94 |
Co—N1 | 2.129 (2) | C1—H1D | 0.91 |
Co—N2 | 2.135 (2) | C2—H2C | 0.96 |
Co—O4iii | 2.1735 (16) | C2—H2D | 0.96 |
N1—C1 | 1.472 (4) | | |
| | | |
O2—Mo—O1 | 108.36 (9) | Coiv—O4—Coi | 95.50 (7) |
O2—Mo—O3 | 109.18 (10) | C1—N1—Co | 107.69 (17) |
O1—Mo—O3 | 109.85 (8) | C1—N1—H1A | 110.1 |
O2—Mo—O4 | 106.94 (8) | Co—N1—H1A | 110.4 |
O1—Mo—O4 | 109.92 (8) | C1—N1—H1B | 110.2 |
O3—Mo—O4 | 112.47 (8) | Co—N1—H1B | 110.5 |
O1—Co—O3i | 98.16 (7) | H1A—N1—H1B | 107.9 |
O1—Co—O4ii | 87.94 (7) | C2—N2—Co | 107.10 (16) |
O3i—Co—O4ii | 90.96 (7) | C2—N2—H2A | 114.3 |
O1—Co—N1 | 173.76 (8) | Co—N2—H2A | 105.8 |
O3i—Co—N1 | 87.69 (8) | C2—N2—H2B | 117.8 |
O4ii—Co—N1 | 94.16 (8) | Co—N2—H2B | 103.8 |
O1—Co—N2 | 95.54 (8) | H2A—N2—H2B | 106.9 |
O3i—Co—N2 | 89.90 (8) | N1—C1—C2 | 110.2 (2) |
O4ii—Co—N2 | 176.27 (8) | N1—C1—H1C | 105.4 |
N1—Co—N2 | 82.25 (9) | C2—C1—H1C | 108.5 |
O1—Co—O4iii | 89.33 (7) | N1—C1—H1D | 111.6 |
O3i—Co—O4iii | 171.11 (7) | C2—C1—H1D | 108.8 |
O4ii—Co—O4iii | 84.50 (7) | H1C—C1—H1D | 112.2 |
N1—Co—O4iii | 85.03 (7) | N2—C2—C1 | 107.9 (2) |
N2—Co—O4iii | 94.16 (7) | N2—C2—H2C | 110.0 |
Mo—O1—Co | 139.83 (11) | C1—C2—H2C | 110.0 |
Mo—O3—Coiii | 146.09 (10) | N2—C2—H2D | 110.1 |
Mo—O4—Coiv | 122.58 (9) | C1—C2—H2D | 110.2 |
Mo—O4—Coi | 130.40 (9) | H2C—C2—H2D | 108.5 |
Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) −x+1, y−1/2, −z+1/2; (iii) x, −y+1/2, z+1/2; (iv) −x+1, y+1/2, −z+1/2. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O1ii | 0.90 | 2.62 | 3.192 (3) | 122 |
N1—H1B···O1v | 0.90 | 2.29 | 3.089 (3) | 148 |
N2—H2A···O2 | 0.90 | 2.40 | 3.127 (3) | 138 |
N2—H2B···O2iii | 0.89 | 2.15 | 3.022 (3) | 167 |
Symmetry codes: (ii) −x+1, y−1/2, −z+1/2; (iii) x, −y+1/2, z+1/2; (v) −x+1, −y, −z+1. |
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