Abstract
In the title molecular salt, (C4H10NO)2[CoCl4], the morpholinium cations adopt chair conformations and the tetrachloridocobaltate(II) anion is significantly distorted from regular tetrahedral geometry [Cl—Co—Cl = 102.183 (19)–117.59 (2)°]. The Co—Cl bond lengths for the chloride ions not accepting hydrogen bonds are significantly shorter than those for the chloride ions accepting such bonds. In the crystal, the components are linked by N—H⋯O and N—H⋯Cl and bifurcated N—H⋯(O,Cl) hydrogen bonds to generate (100) sheets.
Related literature
For a phase transition in morpholinium tetrafluoridoborate, see: Szklarz et al. (2009 ▶); Owczarek et al. (2008 ▶). For the structure of dimorpholinium pentachloridoantimonate(III), see: Chen (2009 ▶).
Experimental
Crystal data
(C4H10NO)2[CoCl4]
M r = 376.99
Monoclinic,
a = 6.5952 (13) Å
b = 13.696 (3) Å
c = 17.039 (3) Å
β = 92.930 (2)°
V = 1537.1 (5) Å3
Z = 4
Mo Kα radiation
μ = 1.80 mm−1
T = 291 K
0.26 × 0.12 × 0.08 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.90, T max = 1.00
11708 measured reflections
2997 independent reflections
2761 reflections with I > 2σ(I)
R int = 0.019
Refinement
R[F 2 > 2σ(F 2)] = 0.022
wR(F 2) = 0.074
S = 1.07
2997 reflections
154 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.42 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); 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: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812035830/hb6916sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812035830/hb6916Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Co1—Cl1 | 2.3029 (6) |
| Co1—Cl2 | 2.2720 (6) |
| Co1—Cl3 | 2.2455 (6) |
| Co1—Cl4 | 2.2811 (6) |
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1C⋯Cl1 | 0.90 | 2.39 | 3.1819 (15) | 148 |
| N1—H1D⋯O2i | 0.90 | 1.97 | 2.8294 (19) | 160 |
| N2—H2C⋯O1ii | 0.90 | 2.47 | 3.0577 (18) | 123 |
| N2—H2C⋯Cl4iii | 0.90 | 2.57 | 3.3322 (15) | 143 |
| N2—H2D⋯Cl1iv | 0.90 | 2.43 | 3.3003 (15) | 164 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
This work was supported by a start-up grant from Jiangsu University of Science and Technology and the Foundation of Jiangsu Educational Committee (grant No. 11KJB150004), China.
supplementary crystallographic information
Experimental
CoCl2 (2.37 g, 10 mmol), morpholine (1.01 g, 10 mmol) and 20% aqueous HCl in a molar ratio of 1:1:1 were mixed and dissolved in sufficient water by heating to 353 K forming a clear solution. The reaction mixture was cooled slowly to room temperature, blue blocks of the title compound were formed, collected and washed with dilute aqueous HCl.
Refinement
All H atoms were placed in calculated positions, with C—H = 0.97 Å and N—H = 0.90 Å, and refined using a riding model, with Uiso(H)=1.2Ueq(C, N).
Figures
Fig. 1.
The asymmetric unit of the title compound. Displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
The packing viewed along the a axis. Hydrogen bonds are drawn as dashed lines
Crystal data
| (C4H10NO)2[CoCl4] | F(000) = 772 |
| Mr = 376.99 | Dx = 1.629 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 2761 reflections |
| a = 6.5952 (13) Å | θ = 2.5–26.0° |
| b = 13.696 (3) Å | µ = 1.80 mm−1 |
| c = 17.039 (3) Å | T = 291 K |
| β = 92.930 (2)° | Block, blue |
| V = 1537.1 (5) Å3 | 0.26 × 0.12 × 0.08 mm |
| Z = 4 |
Data collection
| Rigaku SCXmini diffractometer | 2997 independent reflections |
| Radiation source: fine-focus sealed tube | 2761 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.019 |
| Detector resolution: 13.66612 pixels mm-1 | θmax = 26.0°, θmin = 1.9° |
| ω scans | h = −7→8 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −16→16 |
| Tmin = 0.90, Tmax = 1.00 | l = −20→20 |
| 11708 measured reflections |
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) = 0.074 | H-atom parameters constrained |
| S = 1.07 | w = 1/[σ2(Fo2) + (0.055P)2 + 0.0459P] where P = (Fo2 + 2Fc2)/3 |
| 2997 reflections | (Δ/σ)max = 0.001 |
| 154 parameters | Δρmax = 0.25 e Å−3 |
| 0 restraints | Δρmin = −0.42 e Å−3 |
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 | ||
| C1 | −0.1713 (3) | 0.61037 (13) | 0.55358 (11) | 0.0444 (4) | |
| H1A | −0.2354 | 0.6639 | 0.5801 | 0.053* | |
| H1B | −0.2756 | 0.5629 | 0.5388 | 0.053* | |
| C2 | −0.0788 (3) | 0.64794 (13) | 0.48120 (10) | 0.0404 (4) | |
| H2A | −0.0210 | 0.5943 | 0.4526 | 0.048* | |
| H2B | −0.1819 | 0.6791 | 0.4472 | 0.048* | |
| C3 | 0.2348 (3) | 0.67437 (14) | 0.56019 (11) | 0.0479 (4) | |
| H3A | 0.3349 | 0.7226 | 0.5776 | 0.057* | |
| H3B | 0.3043 | 0.6221 | 0.5342 | 0.057* | |
| C4 | 0.1303 (3) | 0.63460 (14) | 0.62962 (10) | 0.0471 (4) | |
| H4A | 0.2296 | 0.6033 | 0.6653 | 0.056* | |
| H4B | 0.0696 | 0.6880 | 0.6576 | 0.056* | |
| C5 | 1.1478 (3) | 0.07758 (13) | 0.35868 (11) | 0.0472 (4) | |
| H5A | 1.1997 | 0.0142 | 0.3754 | 0.057* | |
| H5B | 1.2597 | 0.1236 | 0.3616 | 0.057* | |
| C6 | 1.0622 (3) | 0.07100 (13) | 0.27501 (11) | 0.0459 (4) | |
| H6A | 1.0223 | 0.1355 | 0.2564 | 0.055* | |
| H6B | 1.1652 | 0.0463 | 0.2415 | 0.055* | |
| C7 | 0.7310 (3) | 0.03294 (13) | 0.32823 (11) | 0.0427 (4) | |
| H7A | 0.6226 | −0.0150 | 0.3280 | 0.051* | |
| H7B | 0.6720 | 0.0957 | 0.3137 | 0.051* | |
| C8 | 0.8328 (3) | 0.03920 (13) | 0.40899 (10) | 0.0428 (4) | |
| H8A | 0.7346 | 0.0588 | 0.4464 | 0.051* | |
| H8B | 0.8854 | −0.0245 | 0.4245 | 0.051* | |
| Cl1 | 0.10686 (6) | 0.80041 (3) | 0.33040 (2) | 0.04020 (12) | |
| Cl2 | 0.55058 (7) | 0.83591 (3) | 0.45501 (2) | 0.04426 (13) | |
| Cl3 | 0.59472 (7) | 0.79781 (4) | 0.23183 (2) | 0.04472 (13) | |
| Cl4 | 0.45151 (7) | 0.59332 (3) | 0.36450 (3) | 0.04461 (13) | |
| Co1 | 0.44468 (3) | 0.757637 (14) | 0.342708 (12) | 0.02945 (10) | |
| N1 | 0.0826 (2) | 0.71964 (10) | 0.50476 (8) | 0.0392 (3) | |
| H1C | 0.1438 | 0.7406 | 0.4618 | 0.047* | |
| H1D | 0.0266 | 0.7716 | 0.5277 | 0.047* | |
| N2 | 0.8819 (2) | 0.00444 (10) | 0.27066 (8) | 0.0395 (3) | |
| H2C | 0.8231 | 0.0064 | 0.2218 | 0.047* | |
| H2D | 0.9231 | −0.0572 | 0.2804 | 0.047* | |
| O1 | −0.02319 (19) | 0.56588 (8) | 0.60621 (7) | 0.0402 (3) | |
| O2 | 0.9955 (2) | 0.10839 (9) | 0.40987 (7) | 0.0454 (3) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0361 (9) | 0.0437 (9) | 0.0533 (11) | −0.0013 (7) | 0.0020 (8) | 0.0055 (8) |
| C2 | 0.0476 (10) | 0.0389 (8) | 0.0335 (9) | 0.0042 (7) | −0.0083 (7) | −0.0026 (7) |
| C3 | 0.0440 (10) | 0.0619 (11) | 0.0373 (9) | −0.0188 (8) | −0.0023 (8) | 0.0045 (8) |
| C4 | 0.0601 (11) | 0.0511 (10) | 0.0292 (9) | −0.0191 (9) | −0.0060 (8) | 0.0041 (7) |
| C5 | 0.0418 (10) | 0.0453 (9) | 0.0544 (11) | −0.0079 (8) | 0.0031 (8) | −0.0097 (8) |
| C6 | 0.0550 (11) | 0.0393 (8) | 0.0448 (10) | −0.0053 (8) | 0.0159 (8) | 0.0002 (8) |
| C7 | 0.0412 (9) | 0.0418 (9) | 0.0450 (10) | −0.0019 (7) | 0.0015 (8) | −0.0046 (7) |
| C8 | 0.0515 (10) | 0.0412 (9) | 0.0363 (9) | −0.0102 (7) | 0.0061 (8) | −0.0041 (7) |
| Cl1 | 0.0353 (2) | 0.0502 (2) | 0.0352 (2) | 0.00980 (16) | 0.00288 (17) | 0.01069 (17) |
| Cl2 | 0.0559 (3) | 0.0427 (2) | 0.0342 (2) | −0.01302 (18) | 0.00315 (19) | −0.00842 (17) |
| Cl3 | 0.0403 (2) | 0.0616 (3) | 0.0330 (2) | −0.00275 (18) | 0.00952 (18) | 0.00554 (18) |
| Cl4 | 0.0543 (3) | 0.0295 (2) | 0.0487 (3) | −0.00623 (16) | −0.0107 (2) | 0.00300 (16) |
| Co1 | 0.03183 (15) | 0.02976 (14) | 0.02686 (15) | −0.00168 (7) | 0.00255 (10) | 0.00081 (7) |
| N1 | 0.0550 (9) | 0.0368 (7) | 0.0266 (7) | −0.0064 (6) | 0.0108 (6) | 0.0019 (6) |
| N2 | 0.0549 (9) | 0.0347 (7) | 0.0283 (7) | 0.0001 (6) | −0.0038 (6) | −0.0015 (5) |
| O1 | 0.0462 (7) | 0.0356 (6) | 0.0384 (6) | −0.0088 (5) | −0.0005 (5) | 0.0075 (5) |
| O2 | 0.0522 (7) | 0.0415 (6) | 0.0428 (7) | −0.0124 (6) | 0.0053 (6) | −0.0148 (5) |
Geometric parameters (Å, º)
| C1—O1 | 1.428 (2) | C6—N2 | 1.497 (2) |
| C1—C2 | 1.495 (2) | C6—H6A | 0.9700 |
| C1—H1A | 0.9700 | C6—H6B | 0.9700 |
| C1—H1B | 0.9700 | C7—N2 | 1.485 (2) |
| C2—N1 | 1.488 (2) | C7—C8 | 1.503 (2) |
| C2—H2A | 0.9700 | C7—H7A | 0.9700 |
| C2—H2B | 0.9700 | C7—H7B | 0.9700 |
| C3—N1 | 1.479 (2) | C8—O2 | 1.431 (2) |
| C3—C4 | 1.502 (2) | C8—H8A | 0.9700 |
| C3—H3A | 0.9700 | C8—H8B | 0.9700 |
| C3—H3B | 0.9700 | Co1—Cl1 | 2.3029 (6) |
| C4—O1 | 1.424 (2) | Co1—Cl2 | 2.2720 (6) |
| C4—H4A | 0.9700 | Co1—Cl3 | 2.2455 (6) |
| C4—H4B | 0.9700 | Co1—Cl4 | 2.2811 (6) |
| C5—O2 | 1.427 (2) | N1—H1C | 0.9000 |
| C5—C6 | 1.509 (3) | N1—H1D | 0.9000 |
| C5—H5A | 0.9700 | N2—H2C | 0.9000 |
| C5—H5B | 0.9700 | N2—H2D | 0.9000 |
| O1—C1—C2 | 111.70 (14) | C5—C6—H6B | 109.7 |
| O1—C1—H1A | 109.3 | H6A—C6—H6B | 108.2 |
| C2—C1—H1A | 109.3 | N2—C7—C8 | 109.66 (14) |
| O1—C1—H1B | 109.3 | N2—C7—H7A | 109.7 |
| C2—C1—H1B | 109.3 | C8—C7—H7A | 109.7 |
| H1A—C1—H1B | 107.9 | N2—C7—H7B | 109.7 |
| N1—C2—C1 | 108.73 (14) | C8—C7—H7B | 109.7 |
| N1—C2—H2A | 109.9 | H7A—C7—H7B | 108.2 |
| C1—C2—H2A | 109.9 | O2—C8—C7 | 110.32 (14) |
| N1—C2—H2B | 109.9 | O2—C8—H8A | 109.6 |
| C1—C2—H2B | 109.9 | C7—C8—H8A | 109.6 |
| H2A—C2—H2B | 108.3 | O2—C8—H8B | 109.6 |
| N1—C3—C4 | 109.34 (15) | C7—C8—H8B | 109.6 |
| N1—C3—H3A | 109.8 | H8A—C8—H8B | 108.1 |
| C4—C3—H3A | 109.8 | Cl3—Co1—Cl2 | 117.59 (2) |
| N1—C3—H3B | 109.8 | Cl3—Co1—Cl4 | 111.892 (19) |
| C4—C3—H3B | 109.8 | Cl2—Co1—Cl4 | 109.01 (2) |
| H3A—C3—H3B | 108.3 | Cl3—Co1—Cl1 | 109.083 (19) |
| O1—C4—C3 | 111.56 (14) | Cl2—Co1—Cl1 | 102.183 (19) |
| O1—C4—H4A | 109.3 | Cl4—Co1—Cl1 | 106.068 (18) |
| C3—C4—H4A | 109.3 | C3—N1—C2 | 110.39 (13) |
| O1—C4—H4B | 109.3 | C3—N1—H1C | 109.6 |
| C3—C4—H4B | 109.3 | C2—N1—H1C | 109.6 |
| H4A—C4—H4B | 108.0 | C3—N1—H1D | 109.6 |
| O2—C5—C6 | 110.74 (15) | C2—N1—H1D | 109.6 |
| O2—C5—H5A | 109.5 | H1C—N1—H1D | 108.1 |
| C6—C5—H5A | 109.5 | C7—N2—C6 | 111.39 (13) |
| O2—C5—H5B | 109.5 | C7—N2—H2C | 109.3 |
| C6—C5—H5B | 109.5 | C6—N2—H2C | 109.3 |
| H5A—C5—H5B | 108.1 | C7—N2—H2D | 109.3 |
| N2—C6—C5 | 109.93 (14) | C6—N2—H2D | 109.3 |
| N2—C6—H6A | 109.7 | H2C—N2—H2D | 108.0 |
| C5—C6—H6A | 109.7 | C4—O1—C1 | 110.33 (13) |
| N2—C6—H6B | 109.7 | C5—O2—C8 | 110.38 (12) |
| O1—C1—C2—N1 | −58.22 (18) | C8—C7—N2—C6 | −53.66 (19) |
| N1—C3—C4—O1 | 57.4 (2) | C5—C6—N2—C7 | 52.48 (19) |
| O2—C5—C6—N2 | −55.95 (19) | C3—C4—O1—C1 | −58.9 (2) |
| N2—C7—C8—O2 | 58.34 (18) | C2—C1—O1—C4 | 59.74 (19) |
| C4—C3—N1—C2 | −56.12 (19) | C6—C5—O2—C8 | 61.60 (19) |
| C1—C2—N1—C3 | 56.46 (18) | C7—C8—O2—C5 | −62.79 (19) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1C···Cl1 | 0.90 | 2.39 | 3.1819 (15) | 148 |
| N1—H1D···O2i | 0.90 | 1.97 | 2.8294 (19) | 160 |
| N2—H2C···O1ii | 0.90 | 2.47 | 3.0577 (18) | 123 |
| N2—H2C···Cl4iii | 0.90 | 2.57 | 3.3322 (15) | 143 |
| N2—H2D···Cl1iv | 0.90 | 2.43 | 3.3003 (15) | 164 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x+1, −y+1/2, z−1/2; (iii) −x+1, y−1/2, −z+1/2; (iv) x+1, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6916).
References
- Chen, L. Z. (2009). Acta Cryst. E65, m689. [DOI] [PMC free article] [PubMed]
- Owczarek, M., Szklarz, P., Jakubas, R. & Lis, T. (2008). Acta Cryst. E64, o667. [DOI] [PMC free article] [PubMed]
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Szklarz, P., Owczarek, M., Bator, G., Lis, T., Gatner, K. & Jakubas, R. (2009). J. Mol. Struct. 929, 48.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812035830/hb6916sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812035830/hb6916Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


