metal-organic compounds
Bis[bis(pentamethylcyclopentadienyl)cobalt(III)] tetrachloridocobaltate(II) dichloromethane disolvate
aDepartment of Chemistry, Virginia Tech, Blacksburg, VA 24061, USA
*Correspondence e-mail: jmerola@vt.edu
The title compound, [Co(C10H15)2]2[CoCl4]·2CH2Cl2, was isolated as a dichloromethane solvate and was formed in the reaction between lithium pentamethylcyclopentadienide and anyhydrous cobalt(II) chloride in tetrahydrofuran. There are two decamethylcobaltocenium cations, one tetrachloridocobaltate(II) anion and two dichloromethane solvent molecules in the formula unit. There is a slight disorder of the dichloromethane solvent which was treated with a two-site model [occupancy rates = 0.765 (4) and 0.235 (4)]. The dichloromethane molecules display significant C—H⋯Cl interactions with the tetrachloridocobaltate(II) dianion. The cobalt atom of the decamethylcobaltocenium cation sits on a twofold rotation axis, with only one pentamethylcyclopentadiene ligand being unique and the second generated by symmetry. The cobalt atom of the [CoCl4]−2 ion sits on a special site with -4 symmetry, with one unique chloride ligand and the others generated by the fourfold inversion axis.
Related literature
For a related structure with a (THF)2LiCl2CoCl2 monoanion and the decamethylcobaltocenium cation, see: Dehnen & Zimmermann (2000) (CCDC 135478). The structure of a related dimer synthesized by Koelle et al. (1986) was determined by Olson & Dahl (1986) (CCDC 566220). For a discussion of the role of chloroform and dichloromethane solvent molecules in crystal packing, see: Allen et al. (2013).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis PRO (Agilent, 2013); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2.
Supporting information
10.1107/S160053681302254X/zl2564sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S160053681302254X/zl2564Isup2.hkl
The procedure described by Koelle et al.(1986) was followed using lithium pentamethylcyclopentadienide (LiCp*) and anhydrous cobalt(II) chloride in tetrahydrofuran. Instead of obtaining the hexane soluble brown dimer as described, the reaction produced a green solid. Dissolution of the solid in dichloromethane followed by slow diffusion of diethyl ether produced well formed green prisms of the title compound that are very air stable and retain the dichloromethane of solvation even after several weeks exposure to the open atmosphere at room temperature.
Data collection: CrysAlis PRO (Agilent, 2013); cell
CrysAlis PRO (Agilent, 2013); data reduction: CrysAlis PRO (Agilent, 2013); program(s) used to solve structure: SHELXS (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).[Co(C10H15)2]2[CoCl4]·2CH2Cl2 | Dx = 1.408 Mg m−3 |
Mr = 1029.32 | Mo Kα radiation, λ = 0.7107 Å |
Tetragonal, P42/n | Cell parameters from 8251 reflections |
a = 12.20980 (12) Å | θ = 4.2–32.2° |
c = 16.2811 (3) Å | µ = 1.48 mm−1 |
V = 2427.17 (7) Å3 | T = 101 K |
Z = 2 | Prism, clear green |
F(000) = 1066 | 0.27 × 0.24 × 0.18 mm |
Agilent Xcalibur (Eos, Gemini ultra) diffractometer | 4161 independent reflections |
Radiation source: Enhance (Mo) X-ray Source | 3394 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.037 |
Detector resolution: 16.0122 pixels mm-1 | θmax = 32.5°, θmin = 3.4° |
ω scans | h = −18→17 |
Absorption correction: gaussian (CrysAlis PRO; Agilent, 2013) | k = −18→12 |
Tmin = 0.755, Tmax = 0.821 | l = −24→21 |
26858 measured reflections |
Refinement on F2 | Primary atom site location: heavy-atom method |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.037 | Hydrogen site location: constr |
wR(F2) = 0.091 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0319P)2 + 2.9104P] where P = (Fo2 + 2Fc2)/3 |
4161 reflections | (Δ/σ)max = 0.001 |
130 parameters | Δρmax = 1.21 e Å−3 |
0 restraints | Δρmin = −1.07 e Å−3 |
[Co(C10H15)2]2[CoCl4]·2CH2Cl2 | Z = 2 |
Mr = 1029.32 | Mo Kα radiation |
Tetragonal, P42/n | µ = 1.48 mm−1 |
a = 12.20980 (12) Å | T = 101 K |
c = 16.2811 (3) Å | 0.27 × 0.24 × 0.18 mm |
V = 2427.17 (7) Å3 |
Agilent Xcalibur (Eos, Gemini ultra) diffractometer | 4161 independent reflections |
Absorption correction: gaussian (CrysAlis PRO; Agilent, 2013) | 3394 reflections with I > 2σ(I) |
Tmin = 0.755, Tmax = 0.821 | Rint = 0.037 |
26858 measured reflections |
R[F2 > 2σ(F2)] = 0.037 | 0 restraints |
wR(F2) = 0.091 | H-atom parameters constrained |
S = 1.04 | Δρmax = 1.21 e Å−3 |
4161 reflections | Δρmin = −1.07 e Å−3 |
130 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 | 0.7500 | 0.2500 | 0.361342 (19) | 0.01381 (8) | |
C1 | 0.86792 (13) | 0.37038 (14) | 0.36190 (10) | 0.0171 (3) | |
C2 | 0.79973 (13) | 0.38033 (14) | 0.29066 (10) | 0.0169 (3) | |
C3 | 0.68885 (14) | 0.39523 (14) | 0.31700 (11) | 0.0193 (3) | |
C4 | 0.68838 (14) | 0.39480 (15) | 0.40471 (11) | 0.0206 (3) | |
C5 | 0.79870 (14) | 0.37984 (14) | 0.43257 (10) | 0.0188 (3) | |
C6 | 0.98932 (14) | 0.35672 (16) | 0.36341 (11) | 0.0221 (3) | |
H6A | 1.0095 | 0.3102 | 0.4085 | 0.033* | |
H6B | 1.0235 | 0.4270 | 0.3699 | 0.033* | |
H6C | 1.0131 | 0.3242 | 0.3128 | 0.033* | |
C7 | 0.83672 (15) | 0.38171 (16) | 0.20305 (11) | 0.0231 (4) | |
H7A | 0.9052 | 0.3436 | 0.1984 | 0.035* | |
H7B | 0.8459 | 0.4561 | 0.1853 | 0.035* | |
H7C | 0.7828 | 0.3464 | 0.1693 | 0.035* | |
C8 | 0.59249 (15) | 0.41374 (17) | 0.26198 (13) | 0.0268 (4) | |
H8A | 0.5987 | 0.3678 | 0.2144 | 0.040* | |
H8B | 0.5906 | 0.4891 | 0.2452 | 0.040* | |
H8C | 0.5263 | 0.3962 | 0.2910 | 0.040* | |
C9 | 0.59133 (16) | 0.41372 (19) | 0.45881 (14) | 0.0318 (4) | |
H9A | 0.5256 | 0.3966 | 0.4292 | 0.048* | |
H9B | 0.5896 | 0.4891 | 0.4756 | 0.048* | |
H9C | 0.5965 | 0.3676 | 0.5064 | 0.048* | |
C10 | 0.83534 (17) | 0.38163 (18) | 0.52022 (12) | 0.0281 (4) | |
H10A | 0.7814 | 0.3462 | 0.5539 | 0.042* | |
H10B | 0.8443 | 0.4561 | 0.5379 | 0.042* | |
H10C | 0.9039 | 0.3437 | 0.5251 | 0.042* | |
Co2 | 1.2500 | 0.2500 | 0.2500 | 0.01550 (10) | |
Cl1 | 1.11315 (3) | 0.29420 (4) | 0.15956 (3) | 0.02050 (9) | |
C11 | 1.2500 | 0.2500 | 0.5298 (2) | 0.0505 (9) | |
H | 1.2150 | 0.1964 | 0.4946 | 0.061* | 0.3825 (19) |
HA | 1.2850 | 0.3036 | 0.4946 | 0.061* | 0.3825 (19) |
HB | 1.2469 | 0.1859 | 0.4946 | 0.061* | 0.1175 (19) |
HC | 1.2531 | 0.3141 | 0.4946 | 0.061* | 0.1175 (19) |
Cl2 | 1.35262 (12) | 0.1830 (2) | 0.58797 (8) | 0.0726 (5) | 0.765 (4) |
Cl2A | 1.3635 (4) | 0.2446 (6) | 0.5851 (3) | 0.0726 (5) | 0.235 (4) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Co1 | 0.01106 (14) | 0.01787 (15) | 0.01251 (14) | 0.00152 (11) | 0.000 | 0.000 |
C1 | 0.0155 (7) | 0.0193 (7) | 0.0167 (7) | −0.0010 (6) | −0.0006 (6) | −0.0008 (6) |
C2 | 0.0162 (7) | 0.0183 (7) | 0.0163 (7) | 0.0004 (6) | −0.0001 (6) | 0.0012 (6) |
C3 | 0.0172 (7) | 0.0186 (7) | 0.0221 (8) | 0.0032 (6) | −0.0017 (6) | −0.0003 (6) |
C4 | 0.0186 (8) | 0.0208 (8) | 0.0224 (8) | 0.0032 (6) | 0.0015 (6) | −0.0042 (6) |
C5 | 0.0177 (7) | 0.0217 (8) | 0.0171 (7) | −0.0002 (6) | 0.0007 (6) | −0.0042 (6) |
C6 | 0.0151 (7) | 0.0317 (9) | 0.0195 (8) | −0.0029 (7) | −0.0005 (6) | 0.0007 (7) |
C7 | 0.0219 (8) | 0.0304 (9) | 0.0169 (8) | −0.0021 (7) | 0.0005 (6) | 0.0031 (7) |
C8 | 0.0191 (8) | 0.0298 (9) | 0.0316 (10) | 0.0068 (7) | −0.0050 (7) | 0.0037 (8) |
C9 | 0.0223 (9) | 0.0390 (11) | 0.0342 (11) | 0.0054 (8) | 0.0083 (8) | −0.0124 (9) |
C10 | 0.0272 (9) | 0.0399 (11) | 0.0171 (8) | −0.0027 (8) | −0.0007 (7) | −0.0060 (8) |
Co2 | 0.01459 (13) | 0.01459 (13) | 0.0173 (2) | 0.000 | 0.000 | 0.000 |
Cl1 | 0.01695 (18) | 0.0238 (2) | 0.02071 (18) | 0.00320 (14) | −0.00162 (14) | −0.00033 (15) |
C11 | 0.056 (2) | 0.069 (3) | 0.0266 (16) | 0.000 (2) | 0.000 | 0.000 |
Cl2 | 0.0681 (7) | 0.0970 (14) | 0.0527 (5) | 0.0388 (9) | −0.0021 (5) | 0.0055 (8) |
Cl2A | 0.0681 (7) | 0.0970 (14) | 0.0527 (5) | 0.0388 (9) | −0.0021 (5) | 0.0055 (8) |
Co1—C1i | 2.0576 (17) | C7—H7B | 0.9600 |
Co1—C1 | 2.0576 (17) | C7—H7C | 0.9600 |
Co1—C2i | 2.0556 (17) | C8—H8A | 0.9600 |
Co1—C2 | 2.0556 (17) | C8—H8B | 0.9600 |
Co1—C3 | 2.0550 (17) | C8—H8C | 0.9600 |
Co1—C3i | 2.0550 (17) | C9—H9A | 0.9600 |
Co1—C4i | 2.0470 (17) | C9—H9B | 0.9600 |
Co1—C4 | 2.0470 (17) | C9—H9C | 0.9600 |
Co1—C5i | 2.0521 (17) | C10—H10A | 0.9600 |
Co1—C5 | 2.0522 (17) | C10—H10B | 0.9600 |
C1—C2 | 1.433 (2) | C10—H10C | 0.9600 |
C1—C5 | 1.432 (2) | Co2—Cl1ii | 2.2915 (4) |
C1—C6 | 1.492 (2) | Co2—Cl1iii | 2.2915 (4) |
C2—C3 | 1.432 (2) | Co2—Cl1 | 2.2915 (4) |
C2—C7 | 1.496 (2) | Co2—Cl1iv | 2.2915 (4) |
C3—C4 | 1.428 (3) | C11—H | 0.9700 |
C3—C8 | 1.496 (2) | C11—HA | 0.9700 |
C4—C5 | 1.433 (2) | C11—HB | 0.9700 |
C4—C9 | 1.494 (3) | C11—HC | 0.9700 |
C5—C10 | 1.496 (3) | C11—Cl2iii | 1.771 (2) |
C6—H6A | 0.9600 | C11—Cl2 | 1.771 (2) |
C6—H6B | 0.9600 | C11—Cl2Aiii | 1.654 (5) |
C6—H6C | 0.9600 | C11—Cl2A | 1.654 (5) |
C7—H7A | 0.9600 | ||
C1—Co1—C1i | 179.49 (9) | C9—C4—Co1 | 128.93 (14) |
C2—Co1—C1i | 139.66 (7) | C1—C5—Co1 | 69.81 (9) |
C2i—Co1—C1i | 40.78 (6) | C1—C5—C4 | 108.10 (15) |
C2—Co1—C1 | 40.78 (6) | C1—C5—C10 | 126.23 (16) |
C2i—Co1—C1 | 139.66 (7) | C4—C5—Co1 | 69.34 (10) |
C2—Co1—C2i | 111.91 (9) | C4—C5—C10 | 125.54 (16) |
C3—Co1—C1i | 111.33 (7) | C10—C5—Co1 | 129.57 (14) |
C3i—Co1—C1i | 68.86 (7) | C1—C6—H6A | 109.5 |
C3i—Co1—C1 | 111.33 (7) | C1—C6—H6B | 109.5 |
C3—Co1—C1 | 68.86 (7) | C1—C6—H6C | 109.5 |
C3i—Co1—C2 | 111.35 (7) | H6A—C6—H6B | 109.5 |
C3—Co1—C2 | 40.77 (7) | H6A—C6—H6C | 109.5 |
C3—Co1—C2i | 111.35 (7) | H6B—C6—H6C | 109.5 |
C3i—Co1—C2i | 40.77 (7) | C2—C7—H7A | 109.5 |
C3—Co1—C3i | 138.87 (10) | C2—C7—H7B | 109.5 |
C4i—Co1—C1 | 110.99 (7) | C2—C7—H7C | 109.5 |
C4—Co1—C1 | 68.82 (7) | H7A—C7—H7B | 109.5 |
C4—Co1—C1i | 110.99 (7) | H7A—C7—H7C | 109.5 |
C4i—Co1—C1i | 68.82 (7) | H7B—C7—H7C | 109.5 |
C4i—Co1—C2i | 68.47 (7) | C3—C8—H8A | 109.5 |
C4i—Co1—C2 | 138.86 (7) | C3—C8—H8B | 109.5 |
C4—Co1—C2 | 68.47 (7) | C3—C8—H8C | 109.5 |
C4—Co1—C2i | 138.86 (7) | H8A—C8—H8B | 109.5 |
C4i—Co1—C3 | 179.56 (8) | H8A—C8—H8C | 109.5 |
C4—Co1—C3 | 40.75 (7) | H8B—C8—H8C | 109.5 |
C4i—Co1—C3i | 40.74 (7) | C4—C9—H9A | 109.5 |
C4—Co1—C3i | 179.56 (8) | C4—C9—H9B | 109.5 |
C4i—Co1—C4 | 139.65 (11) | C4—C9—H9C | 109.5 |
C4i—Co1—C5i | 40.92 (7) | H9A—C9—H9B | 109.5 |
C4i—Co1—C5 | 111.46 (7) | H9A—C9—H9C | 109.5 |
C4—Co1—C5i | 111.46 (7) | H9B—C9—H9C | 109.5 |
C4—Co1—C5 | 40.92 (7) | C5—C10—H10A | 109.5 |
C5—Co1—C1 | 40.79 (7) | C5—C10—H10B | 109.5 |
C5i—Co1—C1 | 138.77 (7) | C5—C10—H10C | 109.5 |
C5i—Co1—C1i | 40.79 (7) | H10A—C10—H10B | 109.5 |
C5—Co1—C1i | 138.77 (7) | H10A—C10—H10C | 109.5 |
C5—Co1—C2i | 179.55 (7) | H10B—C10—H10C | 109.5 |
C5i—Co1—C2i | 68.45 (7) | Cl1iii—Co2—Cl1ii | 114.385 (12) |
C5i—Co1—C2 | 179.55 (7) | Cl1iii—Co2—Cl1 | 100.04 (2) |
C5—Co1—C2 | 68.45 (7) | Cl1ii—Co2—Cl1 | 114.385 (11) |
C5i—Co1—C3 | 139.45 (7) | Cl1iii—Co2—Cl1iv | 114.386 (11) |
C5—Co1—C3 | 68.73 (7) | Cl1ii—Co2—Cl1iv | 100.04 (2) |
C5—Co1—C3i | 139.45 (7) | Cl1—Co2—Cl1iv | 114.385 (11) |
C5i—Co1—C3i | 68.72 (7) | H—C11—HA | 107.5 |
C5i—Co1—C5 | 111.19 (10) | H—C11—HC | 102.2 |
C2—C1—Co1 | 69.54 (9) | HA—C11—HB | 102.2 |
C2—C1—C6 | 126.87 (15) | HB—C11—HC | 107.6 |
C5—C1—Co1 | 69.40 (10) | Cl2iii—C11—H | 108.4 |
C5—C1—C2 | 107.49 (14) | Cl2—C11—H | 108.4 |
C5—C1—C6 | 125.60 (15) | Cl2iii—C11—HA | 108.4 |
C6—C1—Co1 | 127.98 (13) | Cl2—C11—HA | 108.4 |
C1—C2—Co1 | 69.69 (9) | Cl2iii—C11—HB | 131.4 |
C1—C2—C7 | 126.67 (15) | Cl2—C11—HB | 88.3 |
C3—C2—Co1 | 69.59 (10) | Cl2iii—C11—HC | 88.3 |
C3—C2—C1 | 108.52 (14) | Cl2—C11—HC | 131.4 |
C3—C2—C7 | 124.72 (15) | Cl2—C11—Cl2iii | 115.3 (2) |
C7—C2—Co1 | 129.17 (13) | Cl2Aiii—C11—H | 88.8 |
C2—C3—Co1 | 69.64 (9) | Cl2A—C11—H | 131.6 |
C2—C3—C8 | 125.70 (16) | Cl2Aiii—C11—HA | 131.6 |
C4—C3—Co1 | 69.33 (10) | Cl2A—C11—HA | 88.8 |
C4—C3—C2 | 107.63 (15) | Cl2A—C11—HB | 108.7 |
C4—C3—C8 | 126.60 (16) | Cl2Aiii—C11—HB | 108.7 |
C8—C3—Co1 | 128.79 (13) | Cl2A—C11—HC | 108.7 |
C3—C4—Co1 | 69.93 (10) | Cl2Aiii—C11—HC | 108.7 |
C3—C4—C5 | 108.25 (15) | Cl2A—C11—Cl2iii | 108.7 (2) |
C3—C4—C9 | 126.30 (17) | Cl2Aiii—C11—Cl2 | 108.7 (2) |
C5—C4—Co1 | 69.73 (10) | Cl2A—C11—Cl2Aiii | 114.1 (4) |
C5—C4—C9 | 125.35 (17) |
Symmetry codes: (i) −x+3/2, −y+1/2, z; (ii) y+1, −x+3/2, −z+1/2; (iii) −x+5/2, −y+1/2, z; (iv) −y+3/2, x−1, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H···Cl1iv | 0.97 | 2.71 | 3.548 (3) | 145 |
C11—HA···Cl1ii | 0.97 | 2.71 | 3.548 (3) | 145 |
Symmetry codes: (ii) y+1, −x+3/2, −z+1/2; (iv) −y+3/2, x−1, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C11—H···Cl1i | 0.97 | 2.71 | 3.548 (3) | 145.0 |
C11—HA···Cl1ii | 0.97 | 2.71 | 3.548 (3) | 145.0 |
Symmetry codes: (i) −y+3/2, x−1, −z+1/2; (ii) y+1, −x+3/2, −z+1/2. |
Acknowledgements
The authors thank the US National Science Foundation for funding (grant No. CHE-01311288) for the purchase of the Oxford Diffraction Xcalibur2 single-crystal diffractometer.
References
Agilent (2013). CrysAlis PRO. Agilent Technologies UK Ltd, Yarnton, Oxfordshire, England. Google Scholar
Allen, F. H., Wood, P. A. & Galek, P. T. A. (2013). Acta Cryst. B69, 379–388. Web of Science CrossRef CAS IUCr Journals Google Scholar
Dehnen, S. & Zimmermann, C. (2000). Chem. Eur. J. 6, 2256–2261. CrossRef PubMed CAS Google Scholar
Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341. Web of Science CrossRef CAS IUCr Journals Google Scholar
Koelle, U., Fuss, B., Belting, M. & Raabe, E. (1986). Organometallics, 5, 980–987. CSD CrossRef CAS Web of Science Google Scholar
Olson, W. L. & Dahl, L. F. (1986). Acta Cryst. C42, 541–544. CSD CrossRef CAS Web of Science IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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Koelle et al. (1986) reported on the preparation of a pentamethylcyclopentadienylcobalt chloro-bridged dimeric compound that represents an excellent precursor to other mononuclear complexes via bridge-splitting reactions. There is no doubt that Koelle et al. made the described bridged complex since Olson & Dahl (1986) published a crystal structure of the dimer. However, in our laboratories, regardless of the stoichiometry used in attempts to make the chloro bridged dimer described by Koelle et al. (1986), the title compound was the only material isolated. The composition of the title compound consists of two decamethylcobaltocenium cations, one tetrachlorocobalt(II) dianion, and two molecules of dichloromethane. The dichloromethane molecules were slightly disordered and the disorder was treated successfully by a two site model with occupancies of 76.5 (4) and 23.5 (4)%. Dehnen & Zimmerman (2000) noted a similar product in attempts to make selenium-bridged compounds and noted the decamethylcoblatocenium ion was formed depending on the temperature of the reaction. In their case, the CoCl4-2 ion was linked via chloride bridges to a bis-THF Li+ cation.
In the structure reported here, the CoCl4-2 ion shows significant interaction with the dichloromethane of solvation. Recently, Allen et al. (2013) examined the Cambridge Crystallographic Data Base and analyzed crystallographic evidence of C—H···Cl hydrogen bonding for both CH2Cl2 and CHCl3. In that paper, for the specific case of CH2Cl2 interacting with Cl-, they note C—H···Cl interactions with H···Cl distances ranging from 2.33 to 2.95 Å and C—H···Cl angles ranging from 120° to 170° for a set of 63 structures. In the title structure, the H···Cl distance is 2.72 Å with a C—H···Cl angle of 145.0°. These parameters would place the C—H···Cl interaction for the title structure very nearly at the median of the structures analyzed by Allen et al. (2013).
In the structure reported here, the CoCl42- ion is also distorted from perfect tetrahedral geometry with the Cl—Co—Cl angles involved in the hydrogen bonding compressed to 100.04 (2)° and the remaining Cl—Co—Cl angles are 114.385 (12)°. While it is important not to make too much of a qualitative observation, the strength of the C—H···Cl interaction may also be responsible for the relative stability of these crystals in open air. Our experience is that, in the abence of a significant attractive interaction, dichlromethane molecules quite easily evaporate from crystals with loss of crystallinity at room temperature.