Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536801016208/cf6067sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536801016208/cf6067Isup2.hkl |
CCDC reference: 175972
Metallic nickel was electrochemically dissolved in the presence of tetrabutylammonium bromide as supporting electrolyte. Pure nickel foil (AR 99.99%, 2 × 4 × 0.05 cm) was used as cathode and anode. The electrochemical reaction was carried out in a cell without separating the cathode and anode space. 250 ml (2.5 mol) ethanol was poured into the electrolysis bath, as solvent and as reagent. During the electrolysis process, 5 ml (0.05 mol) acetylacetone was gradully added dropwise to the electrolyte. The potential across the anode was adjusted so that a current of 0.2 A passed through the cell for 6 h. Crystals of the title compound were produced.
H atoms bonded to carbon were constrained with a riding model. H atoms of the coordinated water molecules were refined with isotropic displacement parameters, and with restraints on O—H bond lengths, but no H atoms were included for the uncoordinated water.
Data collection: AFC-5R Diffractometer Control Software (Rigaku, 1988); cell refinement: AFC-5R Diffractometer Control Software; data reduction: MolEN/VAX in CAD-4 Operations Manual (Enraf-Nonius, 1977); program(s) used to solve structure: SHELXTL (Sheldrick, 1997); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
[Ni(C5H7O2)2(H2O)2)]·H2O | Z = 2 |
Mr = 310.97 | F(000) = 328 |
Triclinic, P1 | Dx = 1.432 Mg m−3 |
a = 7.5572 (15) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 9.0637 (18) Å | Cell parameters from 20 reflections |
c = 10.997 (2) Å | θ = 15.4–22.9° |
α = 74.17 (3)° | µ = 1.37 mm−1 |
β = 84.50 (3)° | T = 293 K |
γ = 89.74 (3)° | Plate, blue green |
V = 721.2 (2) Å3 | 0.50 × 0.40 × 0.30 mm |
Rigaku AFC-5R diffractometer | 2459 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.036 |
Graphite monochromator | θmax = 26.0°, θmin = 1.9° |
ω/2θ scans | h = −9→9 |
Absorption correction: ψ scan (North et al., 1968) | k = −11→0 |
Tmin = 0.462, Tmax = 0.664 | l = −13→13 |
3104 measured reflections | 3 standard reflections every 300 reflections |
2659 independent reflections | intensity decay: 1.0% |
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)] = 0.040 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.111 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0803P)2 + 0.2124P] where P = (Fo2 + 2Fc2)/3 |
2659 reflections | (Δ/σ)max < 0.001 |
179 parameters | Δρmax = 0.67 e Å−3 |
4 restraints | Δρmin = −0.46 e Å−3 |
[Ni(C5H7O2)2(H2O)2)]·H2O | γ = 89.74 (3)° |
Mr = 310.97 | V = 721.2 (2) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.5572 (15) Å | Mo Kα radiation |
b = 9.0637 (18) Å | µ = 1.37 mm−1 |
c = 10.997 (2) Å | T = 293 K |
α = 74.17 (3)° | 0.50 × 0.40 × 0.30 mm |
β = 84.50 (3)° |
Rigaku AFC-5R diffractometer | 2459 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.036 |
Tmin = 0.462, Tmax = 0.664 | 3 standard reflections every 300 reflections |
3104 measured reflections | intensity decay: 1.0% |
2659 independent reflections |
R[F2 > 2σ(F2)] = 0.040 | 4 restraints |
wR(F2) = 0.111 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | Δρmax = 0.67 e Å−3 |
2659 reflections | Δρmin = −0.46 e Å−3 |
179 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 | ||
Ni | 0.24504 (4) | 0.29439 (3) | 0.04144 (3) | 0.03533 (15) | |
O1 | 0.2319 (3) | 0.1089 (2) | 0.1948 (2) | 0.0528 (5) | |
O2 | 0.2283 (3) | 0.4374 (2) | 0.15143 (19) | 0.0474 (4) | |
O3 | 0.2598 (3) | 0.1575 (2) | −0.07507 (19) | 0.0469 (4) | |
O4 | 0.2615 (3) | 0.4816 (2) | −0.11120 (18) | 0.0487 (5) | |
O5 | 0.5198 (3) | 0.2944 (2) | 0.0411 (3) | 0.0545 (5) | |
O6 | −0.0299 (3) | 0.2886 (2) | 0.0472 (3) | 0.0539 (5) | |
O7 | 0.2386 (3) | −0.1316 (2) | 0.0761 (2) | 0.0604 (6) | |
C1 | 0.2184 (6) | −0.0386 (4) | 0.4070 (3) | 0.0734 (10) | |
H1A | 0.2282 | −0.1195 | 0.3659 | 0.110* | |
H1B | 0.1092 | −0.0518 | 0.4615 | 0.110* | |
H1C | 0.3169 | −0.0418 | 0.4567 | 0.110* | |
C2 | 0.2199 (4) | 0.1143 (3) | 0.3079 (3) | 0.0465 (6) | |
C3 | 0.2078 (4) | 0.2477 (4) | 0.3483 (3) | 0.0539 (7) | |
H3A | 0.1957 | 0.2351 | 0.4355 | 0.065* | |
C4 | 0.2120 (4) | 0.3980 (3) | 0.2707 (3) | 0.0435 (6) | |
C5 | 0.1985 (5) | 0.5279 (4) | 0.3320 (3) | 0.0646 (8) | |
H5A | 0.2031 | 0.6239 | 0.2674 | 0.097* | |
H5B | 0.2957 | 0.5241 | 0.3829 | 0.097* | |
H5C | 0.0881 | 0.5183 | 0.3849 | 0.097* | |
C6 | 0.2857 (6) | 0.0686 (4) | −0.2568 (4) | 0.0744 (10) | |
H6A | 0.2746 | −0.0277 | −0.1925 | 0.112* | |
H6B | 0.3971 | 0.0737 | −0.3079 | 0.112* | |
H6C | 0.1899 | 0.0775 | −0.3095 | 0.112* | |
C7 | 0.2788 (4) | 0.1984 (3) | −0.1944 (3) | 0.0461 (6) | |
C8 | 0.2918 (5) | 0.3496 (4) | −0.2695 (3) | 0.0558 (7) | |
H8A | 0.3085 | 0.3645 | −0.3569 | 0.067* | |
C9 | 0.2821 (4) | 0.4810 (3) | −0.2264 (3) | 0.0458 (6) | |
C10 | 0.2940 (5) | 0.6360 (4) | −0.3221 (3) | 0.0642 (9) | |
H10A | 0.2851 | 0.7147 | −0.2786 | 0.096* | |
H10B | 0.1988 | 0.6451 | −0.3753 | 0.096* | |
H10C | 0.4059 | 0.6471 | −0.3734 | 0.096* | |
H1 | 0.562 (5) | 0.265 (5) | −0.019 (3) | 0.072 (12)* | |
H2 | 0.562 (8) | 0.378 (4) | 0.034 (7) | 0.18 (3)* | |
H3 | −0.073 (6) | 0.364 (4) | 0.061 (5) | 0.102 (16)* | |
H4 | −0.046 (7) | 0.278 (7) | −0.023 (3) | 0.13 (2)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ni | 0.0428 (2) | 0.0247 (2) | 0.0380 (2) | 0.00266 (13) | −0.00507 (14) | −0.00718 (14) |
O1 | 0.0803 (14) | 0.0281 (9) | 0.0469 (11) | 0.0038 (9) | −0.0054 (10) | −0.0053 (8) |
O2 | 0.0679 (12) | 0.0309 (9) | 0.0438 (10) | 0.0024 (8) | −0.0056 (9) | −0.0107 (8) |
O3 | 0.0640 (12) | 0.0308 (9) | 0.0468 (11) | 0.0025 (8) | −0.0048 (9) | −0.0126 (8) |
O4 | 0.0736 (13) | 0.0314 (9) | 0.0390 (10) | 0.0034 (8) | −0.0050 (9) | −0.0065 (8) |
O5 | 0.0440 (10) | 0.0443 (11) | 0.0833 (17) | 0.0032 (9) | −0.0090 (10) | −0.0304 (11) |
O6 | 0.0449 (10) | 0.0436 (11) | 0.0800 (16) | 0.0045 (8) | −0.0060 (10) | −0.0285 (11) |
O7 | 0.0758 (14) | 0.0364 (10) | 0.0716 (14) | 0.0035 (9) | −0.0062 (11) | −0.0195 (10) |
C1 | 0.108 (3) | 0.0433 (17) | 0.0556 (19) | 0.0071 (17) | 0.0002 (19) | 0.0051 (14) |
C2 | 0.0551 (15) | 0.0355 (13) | 0.0433 (14) | 0.0019 (11) | −0.0042 (12) | −0.0013 (11) |
C3 | 0.0724 (19) | 0.0478 (16) | 0.0391 (14) | 0.0031 (14) | −0.0042 (13) | −0.0081 (12) |
C4 | 0.0501 (14) | 0.0421 (14) | 0.0394 (13) | 0.0024 (11) | −0.0047 (11) | −0.0131 (11) |
C5 | 0.090 (2) | 0.0513 (18) | 0.0586 (19) | 0.0061 (16) | −0.0085 (17) | −0.0254 (15) |
C6 | 0.115 (3) | 0.056 (2) | 0.061 (2) | 0.009 (2) | −0.014 (2) | −0.0289 (17) |
C7 | 0.0514 (14) | 0.0426 (14) | 0.0480 (16) | 0.0074 (11) | −0.0116 (12) | −0.0164 (12) |
C8 | 0.076 (2) | 0.0508 (17) | 0.0411 (15) | 0.0061 (15) | −0.0100 (14) | −0.0123 (13) |
C9 | 0.0508 (14) | 0.0408 (14) | 0.0433 (15) | 0.0028 (11) | −0.0085 (11) | −0.0062 (11) |
C10 | 0.091 (2) | 0.0477 (17) | 0.0444 (16) | −0.0005 (16) | −0.0078 (15) | 0.0037 (13) |
Ni—O2 | 1.9958 (19) | C2—C3 | 1.397 (4) |
Ni—O3 | 2.008 (2) | C3—C4 | 1.395 (4) |
Ni—O1 | 2.025 (2) | C3—H3A | 0.930 |
Ni—O4 | 2.030 (2) | C4—C5 | 1.506 (4) |
Ni—O6 | 2.073 (2) | C5—H5A | 0.960 |
Ni—O5 | 2.076 (2) | C5—H5B | 0.960 |
O1—C2 | 1.253 (4) | C5—H5C | 0.960 |
O2—C4 | 1.256 (3) | C6—C7 | 1.513 (4) |
O3—C7 | 1.256 (3) | C6—H6A | 0.960 |
O4—C9 | 1.263 (3) | C6—H6B | 0.960 |
O4—O6i | 2.903 (3) | C6—H6C | 0.960 |
O5—H1 | 0.816 (18) | C7—C8 | 1.392 (4) |
O5—H2 | 0.81 (2) | C8—C9 | 1.396 (4) |
O6—H3 | 0.804 (19) | C8—H8A | 0.930 |
O6—H4 | 0.819 (19) | C9—C10 | 1.505 (4) |
C1—C2 | 1.511 (4) | C10—H10A | 0.960 |
C1—H1A | 0.960 | C10—H10B | 0.960 |
C1—H1B | 0.960 | C10—H10C | 0.960 |
C1—H1C | 0.960 | ||
O2—Ni—O3 | 177.73 (7) | O1—C2—C1 | 115.8 (3) |
O2—Ni—O1 | 91.65 (8) | C3—C2—C1 | 118.6 (3) |
O3—Ni—O1 | 90.55 (8) | C4—C3—C2 | 126.5 (3) |
O2—Ni—O4 | 87.82 (8) | C4—C3—H3A | 116.8 |
O3—Ni—O4 | 89.99 (8) | C2—C3—H3A | 116.8 |
O1—Ni—O4 | 179.09 (8) | O2—C4—C3 | 125.8 (3) |
O2—Ni—O6 | 89.69 (9) | O2—C4—C5 | 115.4 (3) |
O3—Ni—O6 | 89.76 (9) | C3—C4—C5 | 118.8 (3) |
O1—Ni—O6 | 89.64 (10) | C4—C5—H5A | 109.5 |
O4—Ni—O6 | 91.09 (10) | C4—C5—H5B | 109.5 |
O2—Ni—O5 | 90.20 (9) | H5A—C5—H5B | 109.5 |
O3—Ni—O5 | 90.42 (9) | C4—C5—H5C | 109.5 |
O1—Ni—O5 | 88.52 (10) | H5A—C5—H5C | 109.5 |
O4—Ni—O5 | 90.75 (10) | H5B—C5—H5C | 109.5 |
O6—Ni—O5 | 178.15 (9) | C7—C6—H6A | 109.5 |
C2—O1—Ni | 124.88 (18) | C7—C6—H6B | 109.5 |
C4—O2—Ni | 125.48 (17) | H6A—C6—H6B | 109.5 |
C7—O3—Ni | 127.00 (17) | C7—C6—H6C | 109.5 |
C9—O4—Ni | 126.21 (17) | H6A—C6—H6C | 109.5 |
C9—O4—O6i | 117.13 (18) | H6B—C6—H6C | 109.5 |
Ni—O4—O6i | 107.63 (10) | O3—C7—C8 | 125.3 (3) |
Ni—O5—O7ii | 127.64 (11) | O3—C7—C6 | 115.1 (3) |
Ni—O5—H1 | 108 (3) | C8—C7—C6 | 119.7 (3) |
Ni—O5—H2 | 113 (5) | C7—C8—C9 | 126.4 (3) |
H1—O5—H2 | 108 (6) | C7—C8—H8A | 116.8 |
Ni—O6—H3 | 112 (4) | C9—C8—H8A | 116.8 |
Ni—O6—H4 | 102 (4) | O4—C9—C8 | 125.0 (3) |
H3—O6—H4 | 114 (5) | O4—C9—C10 | 115.9 (3) |
C2—C1—H1A | 109.5 | C8—C9—C10 | 119.0 (3) |
C2—C1—H1B | 109.5 | C9—C10—H10A | 109.5 |
H1A—C1—H1B | 109.5 | C9—C10—H10B | 109.5 |
C2—C1—H1C | 109.5 | H10A—C10—H10B | 109.5 |
H1A—C1—H1C | 109.5 | C9—C10—H10C | 109.5 |
H1B—C1—H1C | 109.5 | H10A—C10—H10C | 109.5 |
O1—C2—C3 | 125.6 (3) | H10B—C10—H10C | 109.5 |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O6—H4···O7iii | 0.82 (2) | 2.20 (5) | 2.799 (3) | 130 (5) |
O5—H1···O7ii | 0.82 (2) | 2.08 (3) | 2.781 (3) | 144 (4) |
O6—H3···O4i | 0.80 (2) | 2.13 (2) | 2.903 (3) | 161 (5) |
O5—H2···O2iv | 0.81 (2) | 2.65 (5) | 3.237 (3) | 131 (6) |
O5—H2···O4iv | 0.81 (2) | 2.22 (4) | 2.929 (3) | 147 (6) |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y, −z; (iii) −x, −y, −z; (iv) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | [Ni(C5H7O2)2(H2O)2)]·H2O |
Mr | 310.97 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 293 |
a, b, c (Å) | 7.5572 (15), 9.0637 (18), 10.997 (2) |
α, β, γ (°) | 74.17 (3), 84.50 (3), 89.74 (3) |
V (Å3) | 721.2 (2) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 1.37 |
Crystal size (mm) | 0.50 × 0.40 × 0.30 |
Data collection | |
Diffractometer | Rigaku AFC-5R diffractometer |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.462, 0.664 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3104, 2659, 2459 |
Rint | 0.036 |
(sin θ/λ)max (Å−1) | 0.617 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.040, 0.111, 1.04 |
No. of reflections | 2659 |
No. of parameters | 179 |
No. of restraints | 4 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.67, −0.46 |
Computer programs: AFC-5R Diffractometer Control Software (Rigaku, 1988), AFC-5R Diffractometer Control Software, MolEN/VAX in CAD-4 Operations Manual (Enraf-Nonius, 1977), SHELXTL (Sheldrick, 1997), SHELXTL.
Ni—O2 | 1.9958 (19) | Ni—O4 | 2.030 (2) |
Ni—O3 | 2.008 (2) | Ni—O6 | 2.073 (2) |
Ni—O1 | 2.025 (2) | Ni—O5 | 2.076 (2) |
O2—Ni—O3 | 177.73 (7) | O1—Ni—O6 | 89.64 (10) |
O2—Ni—O1 | 91.65 (8) | O4—Ni—O6 | 91.09 (10) |
O3—Ni—O1 | 90.55 (8) | O2—Ni—O5 | 90.20 (9) |
O2—Ni—O4 | 87.82 (8) | O3—Ni—O5 | 90.42 (9) |
O3—Ni—O4 | 89.99 (8) | O1—Ni—O5 | 88.52 (10) |
O1—Ni—O4 | 179.09 (8) | O4—Ni—O5 | 90.75 (10) |
O2—Ni—O6 | 89.69 (9) | O6—Ni—O5 | 178.15 (9) |
O3—Ni—O6 | 89.76 (9) |
D—H···A | D—H | H···A | D···A | D—H···A |
O6—H4···O7i | 0.819 (19) | 2.20 (5) | 2.799 (3) | 130 (5) |
O5—H1···O7ii | 0.816 (18) | 2.08 (3) | 2.781 (3) | 144 (4) |
O6—H3···O4iii | 0.804 (19) | 2.13 (2) | 2.903 (3) | 161 (5) |
O5—H2···O2iv | 0.81 (2) | 2.65 (5) | 3.237 (3) | 131 (6) |
O5—H2···O4iv | 0.81 (2) | 2.22 (4) | 2.929 (3) | 147 (6) |
Symmetry codes: (i) −x, −y, −z; (ii) −x+1, −y, −z; (iii) −x, −y+1, −z; (iv) −x+1, −y+1, −z. |
The paramagnetic complex Ni(acac)2(H2O)2 (acac = acetylacetonato) has been a subject of interest to chemists for the past two decades (Abernathy & Sharp, 1997; Sharp et al., 1997; Miller et al., 2000; Lorh et al., 1999), following the earlier report of trinuclear molecules in the crystal structure of Ni(acac)2 (Bullen, 1956). Paramagnetic transition metal ions in solution can produce large nuclear magnetic resonance (NMR) relaxation enhancements of nuclear spins in ligand species and in solvent molecules. This phenomenon, called NMR paramagnetic relaxation enhancement or NMR–PRE, has been used widely to probe the structure, dynamics and magnetic properties of dissolved paramagnetic species. Crystal structures of suitable paramagnetic complexes provide structural data to aid NMR–PRE study (Sharp et al., 1997).
Recently, electrochemical dissolution of a nickel anode in acetylacetone and ethanol solution was carried out in our laboratory (Zhou et al., 2000a,b, 2001). Some water was added to the electrolyte to produce hydrolysis and prepare nanometer NiO by a sol–gel process at room temperature. The complex Ni(acac)2(H2O)2 crystallized out of the solution.
The molecular structure is essentially the same as that reported by Montgomery & Lingafelter (1964) for this complex without water of crystallization. Though Misra et al. (1979) considered it was not possible to produce a single-crystal of Ni(acac)2(H2O)2, it was very easy for us to obtain by using an electrochemical method. Because of our interest in sol–gel chemistry, the electrolyte solution with some added water was heated to 333 K for 30 min. Crystals of hydrated Ni(acac)2(H2O)2.H2O, (I), were also obtained and the crystal structure has been determined. Each of the two products can be obtained preferentially by controlling the hydrolysis temperature carefully. Harlow & Pfluger (1973) obtained crystals of the hydrate by using a completely different method previously. The structure reported here is of greater precision.
Selected bond lengths and angles are given in Table 1, and the molecular structure is shown in Fig. 1, with a packing diagram shown in Fig. 2. The uncoordinated water molecule is involved in hydrogen bonding, and further hydrogen bonding links coordinated water molecules to acac ligands in adjacent molecules (Table 2).
In the structure without water of crystallization, the nickel ion has acac O atoms at 2.021 and 2.014 Å and water O atoms at 2.139 Å in a precisely centrosymmetric arrangement. In the hydrated structure, the corresponding distances are 1.994 (2)–2.031 (2) Å for acac, and 2.075 (2) and 2.080 (2) Å for water ligands, respectively, the nickel ion lying in a general position but retaining an octahedral coordination.