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The crystal structure of tetra-aqua-bis(acetato-O)cobalt(II), Co(C2H3O2)2(H2O)4, has been determined at 153 K, providing a precise description of the geometric parameters and details of the hydrogen-bonding system operating in the crystal.
Supporting information
CCDC reference: 225647
Key indicators
- Single-crystal X-ray study
- T = 153 K
- Mean (C-C) = 0.001 Å
- R factor = 0.018
- wR factor = 0.047
- Data-to-parameter ratio = 27.0
checkCIF/PLATON results
No syntax errors found
Alert level B
PLAT232_ALERT_2_B Hirshfeld Test Diff (M-X) Co - O3 = 14.42 su
Alert level C
PLAT029_ALERT_3_C _diffrn_measured_fraction_theta_full Low ....... 0.99
PLAT164_ALERT_4_C Nr. of Refined C-H H-Atoms in Heavy-At Struct... 3
PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Co - O1 = 9.35 su
PLAT232_ALERT_2_C Hirshfeld Test Diff (M-X) Co - O4 = 9.58 su
0 ALERT level A = In general: serious problem
1 ALERT level B = Potentially serious problem
4 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
3 ALERT type 2 Indicator that the structure model may be wrong or deficient
1 ALERT type 3 Indicator that the structure quality may be low
1 ALERT type 4 Improvement, methodology, query or suggestion
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Bruker, 1997); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Crystal data top
[Co(C2H3O2)2(H2O)4] | F(000) = 258 |
Mr = 249.08 | Dx = 1.767 Mg m−3 |
Monoclinic, P21/c | Melting point: not measured K |
Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
a = 4.7744 (3) Å | Cell parameters from 6622 reflections |
b = 11.8425 (8) Å | θ = 3.0–37.5° |
c = 8.2904 (6) Å | µ = 1.85 mm−1 |
β = 93.142 (2)° | T = 153 K |
V = 468.04 (5) Å3 | Cuboid, pink |
Z = 2 | 0.48 × 0.42 × 0.38 mm |
Data collection top
Bruker AXS CCD diffractometer | 2429 independent reflections |
Radiation source: sealed tube | 2241 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
ω scans | θmax = 37.5°, θmin = 3.0° |
Absorption correction: multi-scan (SADABS; Bruker, 1997) | h = −8→7 |
Tmin = 0.430, Tmax = 0.499 | k = 0→20 |
9443 measured reflections | l = 0→14 |
Refinement top
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.018 | All H-atom parameters refined |
wR(F2) = 0.047 | w = 1/[σ2(Fo2) + (0.0215P)2 + 0.1094P] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max < 0.001 |
2429 reflections | Δρmax = 0.47 e Å−3 |
90 parameters | Δρmin = −0.46 e Å−3 |
0 restraints | Extinction correction: SHELXTL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.041 (2) |
Special details top
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 | |
Co | 0.0000 | 0.0000 | 0.0000 | 0.00986 (4) | |
O1 | −0.23355 (10) | 0.14910 (4) | 0.01084 (6) | 0.01385 (8) | |
O2 | 0.07771 (11) | 0.25626 (4) | 0.14962 (7) | 0.01853 (10) | |
C1 | −0.13738 (12) | 0.24507 (5) | 0.05703 (7) | 0.01229 (9) | |
C2 | −0.28889 (16) | 0.34804 (6) | −0.00700 (9) | 0.01865 (12) | |
H21 | −0.237 (3) | 0.4141 (13) | 0.0513 (18) | 0.039 (4)* | |
H22 | −0.480 (3) | 0.3386 (17) | −0.0043 (18) | 0.047 (5)* | |
H23 | −0.244 (4) | 0.3592 (14) | −0.113 (2) | 0.051 (5)* | |
O3 | 0.24129 (10) | 0.04740 (4) | 0.20619 (6) | 0.01468 (8) | |
H31 | 0.223 (3) | 0.1168 (13) | 0.2040 (18) | 0.037 (4)* | |
H32 | 0.405 (3) | 0.0272 (12) | 0.2075 (18) | 0.030 (3)* | |
O4 | 0.28363 (10) | 0.08242 (4) | −0.14784 (6) | 0.01324 (8) | |
H41 | 0.409 (3) | 0.1183 (12) | −0.0995 (17) | 0.035 (3)* | |
H42 | 0.214 (3) | 0.1293 (12) | −0.2165 (17) | 0.034 (3)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Co | 0.00836 (5) | 0.00904 (5) | 0.01195 (5) | −0.00016 (3) | −0.00149 (3) | −0.00024 (3) |
O1 | 0.01142 (18) | 0.01059 (17) | 0.0192 (2) | −0.00011 (13) | −0.00258 (14) | −0.00179 (15) |
O2 | 0.0168 (2) | 0.0139 (2) | 0.0240 (2) | 0.00023 (16) | −0.00709 (17) | −0.00448 (17) |
C1 | 0.0121 (2) | 0.0109 (2) | 0.0139 (2) | 0.00058 (17) | 0.00055 (17) | −0.00111 (17) |
C2 | 0.0212 (3) | 0.0124 (2) | 0.0220 (3) | 0.0038 (2) | −0.0015 (2) | 0.0007 (2) |
O3 | 0.01304 (19) | 0.0145 (2) | 0.01613 (19) | 0.00094 (15) | −0.00290 (15) | −0.00142 (15) |
O4 | 0.01089 (17) | 0.01260 (18) | 0.01591 (19) | −0.00083 (14) | −0.00217 (14) | 0.00264 (15) |
Geometric parameters (Å, º) top
Co—O1 | 2.0929 (5) | C1—C2 | 1.5001 (9) |
Co—O1i | 2.0929 (5) | C2—H21 | 0.946 (15) |
Co—O3 | 2.0853 (5) | C2—H22 | 0.921 (15) |
Co—O3i | 2.0853 (5) | C2—H23 | 0.929 (16) |
Co—O4 | 2.1144 (5) | O3—H31 | 0.827 (15) |
Co—O4i | 2.1144 (5) | O3—H32 | 0.817 (15) |
O1—C1 | 1.2767 (8) | O4—H41 | 0.821 (15) |
O2—C1 | 1.2550 (8) | O4—H42 | 0.849 (15) |
| | | |
O1—Co—O3 | 90.54 (2) | O2—C1—O1 | 123.11 (6) |
O1—Co—O4 | 89.72 (2) | O2—C1—C2 | 119.55 (6) |
O3—Co—O4 | 90.48 (2) | O1—C1—C2 | 117.32 (6) |
O1i—Co—O1 | 180.0 | C1—C2—H21 | 112.6 (9) |
O1—Co—O3i | 89.46 (2) | C1—C2—H22 | 110.6 (12) |
O1—Co—O4i | 90.28 (2) | H21—C2—H22 | 108.7 (14) |
O3—Co—O4i | 89.52 (2) | C1—C2—H23 | 108.6 (10) |
O3—Co—O3i | 180.0 | H21—C2—H23 | 107.4 (14) |
O1i—Co—O3 | 89.46 (2) | H22—C2—H23 | 108.8 (14) |
O1i—Co—O4 | 90.28 (2) | Co—O3—H31 | 101.3 (10) |
O3i—Co—O4 | 89.52 (2) | Co—O3—H32 | 114.6 (10) |
O4i—Co—O4 | 180.0 | H31—O3—H32 | 113.2 (14) |
O1i—Co—O3i | 90.54 (2) | Co—O4—H41 | 115.5 (9) |
O1i—Co—O4i | 89.72 (2) | Co—O4—H42 | 116.8 (9) |
O3i—Co—O4i | 90.48 (2) | H41—O4—H42 | 103.7 (13) |
C1—O1—Co | 125.47 (4) | | |
Symmetry code: (i) −x, −y, −z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O3—H31···O2 | 0.83 (2) | 1.84 (2) | 2.6282 (8) | 160 (2) |
O3—H32···O4ii | 0.82 (2) | 2.05 (2) | 2.8041 (7) | 153 (1) |
O4—H41···O1iii | 0.82 (2) | 1.93 (2) | 2.7084 (7) | 159 (1) |
O4—H42···O2iv | 0.85 (2) | 1.85 (2) | 2.6935 (7) | 174 (1) |
Symmetry codes: (ii) −x+1, −y, −z; (iii) x+1, y, z; (iv) x, −y+1/2, z−1/2. |
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