metal-organic compounds
catena-poly[[[diaquacobalt(II)]-bis(μ-hex-3-enedinitrile-κ2N:N′)] bis(tetrafluoridoborate)]
ofaDaegu Gyeongbuk Institue of Science & Technology (DGIST), Daegu 711-873, Republic of Korea
*Correspondence e-mail: dukelee@dgist.ac.kr, st.hong@dgist.ac.kr
In the structure of the title salt, [Co(C6H6N2)2(H2O)2](BF4)2, the CoII atom is located on an inversion centre. The transition metal is in a slightly distorted octahedral coordination environment, defined by the cyano N atoms of four hex-3-enedinitrile ligands in equatorial positions and the O atoms of two water molecules in axial positions. The bridging mode of the hex-3-enedinitrile ligands leads to the formation of cationic chains extending parallel to [1-10]. The BF4− counter-anion is disordered over two sets of sites [occupancy ratio = 0.512 (19):0.489 (19)]. It is located in the voids between the cationic chains and is connected to the aqua ligands of the latter through O—H⋯F hydrogen bonds. One methylene H atom of the hex-3-enedinitrile ligand forms another and weak C—H⋯O hydrogen bond with a water O atom of a neighbouring chain, thus consolidating the three-dimensional network structure.
Keywords: crystal structure; cobalt; hex-3-enedinitrile; hydrogen bonding.
CCDC reference: 1401602
1. Related literature
Aliphatic dinitriles have gained much attention not only due to their rich coordination chemistry with transition-metal ions (Storhoff & Lewis, 1977; Heller & Sheldrick, 2004; Blount et al., 1969), but also due to their applications as functional electrolyte additives for lithium ion batteries (Kim et al., 2011, 2014a,b). While the coordination complexes of saturated aliphatic dinitrile ligands have been extensively studied (Storhoff & Lewis, 1977; Heller & Sheldrick, 2004; Blount et al., 1969), those of unsaturated dinitrile ligands like in the title compound have hardly been reported so far.
2. Experimental
2.1. Crystal data
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2.3. Refinement
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Data collection: APEX2 (Bruker, 2006); cell SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: ATOMS (Dowty, 2000); software used to prepare material for publication: CRYSTALS.
Supporting information
CCDC reference: 1401602
10.1107/S2056989015009548/wm5160sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2056989015009548/wm5160Isup2.hkl
A solvent was prepared first by mixing ethylene carbonate (EC) and ethyl methyl carbonate (EMC) in an 1:2 volume ratio (3.3 ml and 6.6 ml, respectively). 0.934 g of lithium tetrafluoridoborate (LiBF4) were added to the solvent, and it was stirred for about 5 hours to dissolve the salt completely to form an 1M solution. 0.60 g (5 wt.%) of cobalt(II) tetrafluoridoborate hexahydrate and 0.24 g (2 wt.%) hex-3-enedinitrile were added and dissolved in the solution. The solution was kept for 48 hours in an argon-atmosphere glove-box at room temperature, resulting in the growth of red crystals. The crystals were washed with pure EMC solvent three times in the argon-atmosphere glove-box.
H atoms attached to C atoms of the title compound were placed in geometrically idealized positions and treated as rigid bodies with C—H distances constrained to 0.92–0.97 Å. Water H atoms were located from a difference map and refined with a distance of 0.82 Å. The BF4- counter anion was refined with a positional disorder model where F2, F3 and F4 atoms are split into two positions while B1 and F1 atoms are not. Such a disorder model resulted in a slightly better
reducing the R1 factor values from 0.041 to 0.033.Data collection: APEX2 (Bruker, 2006); cell
SAINT (Bruker, 2006); data reduction: SAINT (Bruker, 2006); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: ATOMS (Dowty, 2000); software used to prepare material for publication: CRYSTALS (Betteridge et al., 2003).[Co(C6H6N2)(H2O)2](BF4)2 | Z = 1 |
Mr = 480.84 | F(000) = 241 |
Triclinic, P1 | Dx = 1.575 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.9839 (11) Å | Cell parameters from 0 reflections |
b = 8.3434 (11) Å | θ = 0–0° |
c = 8.8441 (13) Å | µ = 0.93 mm−1 |
α = 71.380 (5)° | T = 103 K |
β = 88.458 (5)° | Cuboid, yellow |
γ = 66.184 (4)° | 0.20 × 0.20 × 0.20 mm |
V = 507.21 (12) Å3 |
Bruker APEXII CCD diffractometer | 2233 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.038 |
ϕ & ω scans | θmax = 28.5°, θmin = 2.8° |
Absorption correction: multi-scan (SADABS; Bruker, 2006) | h = −10→10 |
Tmin = 0.60, Tmax = 0.75 | k = −11→11 |
14705 measured reflections | l = −11→11 |
2501 independent reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.033 | H-atom parameters constrained |
wR(F2) = 0.068 | Weighting scheme based on measured s.u.'s W = 1 |
S = 0.87 | (Δ/σ)max = 0.0002 |
2202 reflections | Δρmax = 0.83 e Å−3 |
170 parameters | Δρmin = −0.62 e Å−3 |
20 restraints |
[Co(C6H6N2)(H2O)2](BF4)2 | γ = 66.184 (4)° |
Mr = 480.84 | V = 507.21 (12) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.9839 (11) Å | Mo Kα radiation |
b = 8.3434 (11) Å | µ = 0.93 mm−1 |
c = 8.8441 (13) Å | T = 103 K |
α = 71.380 (5)° | 0.20 × 0.20 × 0.20 mm |
β = 88.458 (5)° |
Bruker APEXII CCD diffractometer | 2501 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2006) | 2233 reflections with I > 2σ(I) |
Tmin = 0.60, Tmax = 0.75 | Rint = 0.038 |
14705 measured reflections |
R[F2 > 2σ(F2)] = 0.033 | 20 restraints |
wR(F2) = 0.068 | H-atom parameters constrained |
S = 0.87 | Δρmax = 0.83 e Å−3 |
2202 reflections | Δρmin = −0.62 e Å−3 |
170 parameters |
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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.0000 | 1.0000 | 0.5000 | 0.0158 | |
N1 | 0.2687 (2) | 0.8866 (2) | 0.6299 (2) | 0.0199 | |
N2 | 0.1190 (2) | 0.9254 (2) | 0.3036 (2) | 0.0192 | |
C1 | 0.4140 (2) | 0.8397 (3) | 0.6904 (2) | 0.0179 | |
C2 | 0.6004 (3) | 0.7780 (3) | 0.7691 (3) | 0.0221 | |
C3 | 0.7036 (2) | 0.5683 (3) | 0.8382 (2) | 0.0200 | |
C4 | 0.6448 (3) | 0.4468 (3) | 0.8245 (2) | 0.0201 | |
C5 | 0.7535 (3) | 0.2388 (3) | 0.9045 (2) | 0.0244 | |
C6 | 0.8244 (2) | 0.1444 (2) | 0.7878 (2) | 0.0181 | |
O1 | 0.02105 (18) | 1.25018 (18) | 0.41358 (16) | 0.0197 | |
B1 | 0.7569 (3) | 0.7200 (3) | 0.2131 (3) | 0.0287 | |
F1 | 0.77132 (18) | 0.55820 (17) | 0.18696 (15) | 0.0295 | |
F2 | 0.8571 (16) | 0.6724 (15) | 0.3523 (13) | 0.0555 | 0.512 (19) |
F3 | 0.8368 (13) | 0.8076 (13) | 0.0834 (11) | 0.0630 | 0.512 (19) |
F4 | 0.5804 (9) | 0.8300 (10) | 0.2014 (15) | 0.0585 | 0.512 (19) |
F21 | 0.9052 (8) | 0.6606 (13) | 0.3357 (11) | 0.0255 | 0.489 (19) |
F31 | 0.7671 (17) | 0.8497 (11) | 0.0853 (10) | 0.0551 | 0.489 (19) |
F41 | 0.5866 (9) | 0.7929 (11) | 0.2810 (16) | 0.0534 | 0.489 (19) |
H11 | 0.0413 | 1.2954 | 0.4771 | 0.034 (4)* | |
H12 | −0.0554 | 1.3393 | 0.3416 | 0.043 (4)* | |
H21 | 0.5897 | 0.8291 | 0.8529 | 0.034 (4)* | |
H22 | 0.6694 | 0.8293 | 0.6919 | 0.033 (4)* | |
H31 | 0.8174 | 0.5253 | 0.8931 | 0.034 (4)* | |
H41 | 0.5301 | 0.4889 | 0.7639 | 0.035 (4)* | |
H51 | 0.6801 | 0.1848 | 0.9680 | 0.036 (4)* | |
H52 | 0.8570 | 0.2189 | 0.9701 | 0.034 (4)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.01363 (18) | 0.01074 (17) | 0.0198 (2) | −0.00181 (13) | −0.00123 (13) | −0.00526 (14) |
N1 | 0.0166 (8) | 0.0169 (8) | 0.0222 (8) | −0.0025 (6) | −0.0014 (6) | −0.0070 (6) |
N2 | 0.0170 (7) | 0.0163 (8) | 0.0211 (8) | −0.0039 (6) | 0.0006 (6) | −0.0060 (6) |
C1 | 0.0173 (7) | 0.0138 (8) | 0.0201 (9) | −0.0033 (7) | 0.0015 (7) | −0.0067 (7) |
C2 | 0.0153 (7) | 0.0209 (9) | 0.0292 (10) | −0.0055 (7) | −0.0023 (7) | −0.0093 (8) |
C3 | 0.0139 (7) | 0.0221 (9) | 0.0194 (9) | −0.0018 (7) | −0.0025 (7) | −0.0081 (7) |
C4 | 0.0170 (7) | 0.0207 (9) | 0.0178 (9) | −0.0024 (7) | 0.0018 (7) | −0.0076 (7) |
C5 | 0.0266 (7) | 0.0216 (10) | 0.0182 (9) | −0.0031 (8) | 0.0026 (8) | −0.0074 (8) |
C6 | 0.0172 (7) | 0.0135 (8) | 0.0176 (9) | −0.0032 (7) | −0.0023 (7) | −0.0015 (7) |
O1 | 0.0223 (7) | 0.0126 (6) | 0.0219 (7) | −0.0052 (5) | −0.0021 (5) | −0.0056 (5) |
B1 | 0.0252 (12) | 0.0159 (10) | 0.0380 (14) | −0.0057 (9) | −0.0119 (10) | −0.0028 (10) |
F1 | 0.0363 (7) | 0.0211 (6) | 0.0283 (7) | −0.0096 (5) | −0.0101 (5) | −0.0067 (5) |
F2 | 0.072 (4) | 0.036 (3) | 0.049 (4) | −0.010 (4) | −0.032 (4) | −0.017 (2) |
F3 | 0.046 (3) | 0.047 (4) | 0.071 (3) | −0.026 (3) | −0.009 (3) | 0.022 (3) |
F4 | 0.0361 (18) | 0.039 (3) | 0.088 (5) | 0.0039 (18) | 0.000 (3) | −0.031 (3) |
F21 | 0.0208 (19) | 0.021 (2) | 0.032 (2) | −0.0030 (16) | −0.0089 (16) | −0.0115 (15) |
F31 | 0.072 (4) | 0.031 (3) | 0.046 (2) | −0.028 (3) | −0.025 (3) | 0.019 (2) |
F41 | 0.0304 (19) | 0.042 (3) | 0.088 (5) | −0.0067 (18) | 0.010 (3) | −0.034 (3) |
Co1—N1i | 2.1486 (17) | C4—H41 | 0.946 |
Co1—N2i | 2.1050 (17) | C5—C6 | 1.460 (6) |
Co1—O1i | 2.0560 (15) | C5—H51 | 0.946 |
Co1—N1 | 2.1486 (17) | C5—H52 | 0.949 |
Co1—N2 | 2.1050 (17) | O1—H11 | 0.821 |
Co1—O1 | 2.0560 (15) | O1—H12 | 0.826 |
N1—C1 | 1.148 (6) | B1—F1 | 1.401 (3) |
N2—C6ii | 1.125 (5) | B1—F2 | 1.341 (12) |
C1—C2 | 1.474 (8) | B1—F3 | 1.435 (11) |
C2—C3 | 1.514 (9) | B1—F4 | 1.320 (9) |
C2—H21 | 0.953 | B1—F1 | 1.401 (3) |
C2—H22 | 0.967 | B1—F21 | 1.440 (12) |
C3—C4 | 1.315 (4) | B1—F31 | 1.319 (11) |
C3—H31 | 0.916 | B1—F41 | 1.450 (10) |
C4—C5 | 1.516 (3) | ||
N1i—Co1—N2i | 90.57 (6) | C4—C3—H31 | 118.7 |
N1i—Co1—O1i | 87.29 (6) | C3—C4—C5 | 122.3 (3) |
N2i—Co1—O1i | 91.15 (6) | C3—C4—H41 | 119.7 |
N1i—Co1—N1 | 179.995 | C5—C4—H41 | 118.0 |
N2i—Co1—N1 | 89.4 (8) | C4—C5—C6 | 112.18 (14) |
O1i—Co1—N1 | 92.7 (4) | C4—C5—H51 | 110.9 |
N1i—Co1—N2 | 89.4 (4) | C6—C5—H51 | 108.7 |
N2i—Co1—N2 | 179.995 | C4—C5—H52 | 108.2 |
O1i—Co1—N2 | 88.9 (6) | C6—C5—H52 | 107.0 |
N1—Co1—N2 | 90.57 (6) | H51—C5—H52 | 109.8 |
N1i—Co1—O1 | 92.7 (8) | C5—C6—N2ii | 178.3 (2) |
N2i—Co1—O1 | 88.9 (3) | Co1—O1—H11 | 119.4 |
O1i—Co1—O1 | 179.994 | Co1—O1—H12 | 121.0 |
N1—Co1—O1 | 87.29 (6) | H11—O1—H12 | 105.0 |
N2—Co1—O1 | 91.15 (6) | F1—B1—F2 | 109.0 (6) |
Co1—N1—C1 | 173.92 (16) | F1—B1—F3 | 105.3 (7) |
Co1—N2—C6ii | 166.34 (18) | F2—B1—F3 | 109.1 (7) |
N1—C1—C2 | 179.5 (2) | F1—B1—F4 | 108.3 (6) |
C1—C2—C3 | 113.2 (2) | F2—B1—F4 | 115.9 (6) |
C1—C2—H21 | 108.5 | F3—B1—F4 | 108.7 (6) |
C3—C2—H21 | 109.3 | F1—B1—F21 | 105.8 (6) |
C1—C2—H22 | 108.7 | F1—B1—F31 | 115.0 (6) |
C3—C2—H22 | 109.9 | F21—B1—F31 | 109.8 (7) |
H21—C2—H22 | 107.0 | F1—B1—F41 | 108.4 (6) |
C2—C3—C4 | 125.87 (19) | F21—B1—F41 | 106.8 (6) |
C2—C3—H31 | 115.5 | F31—B1—F41 | 110.7 (8) |
Symmetry codes: (i) −x, −y+2, −z+1; (ii) −x+1, −y+1, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H22···O1iii | 0.97 | 2.52 | 3.348 (3) | 143 (1) |
O1—H12···F1iv | 0.83 | 1.89 | 2.72 (2) | 175 (1) |
O1—H11···F2iii | 0.82 | 1.87 | 2.669 (13) | 163 (1) |
Symmetry codes: (iii) −x+1, −y+2, −z+1; (iv) x−1, y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C2—H22···O1i | 0.970 | 2.520 | 3.348 (3) | 143.1 (3) |
O1—H12···F1ii | 0.830 | 1.890 | 2.72 (2) | 174.58 (8) |
O1—H11···F2i | 0.820 | 1.873 | 2.669 (13) | 163.0 (4) |
Symmetry codes: (i) −x+1, −y+2, −z+1; (ii) x−1, y+1, z. |
Footnotes
‡contributed equally.
Acknowledgements
This work was supported by the DGIST R&D Program of Ministry of Science, ICT and Future Planning of Korea (grant No. 15-HRLA-01).
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