Abstract
The title complex, [Cu(C11H10N2O2)2](BF4)2·2H2O, was isolated as a dihydrate from a 1:2 molar mixture of copper(II) tetrafluoridoborate hexahydrate with di-2-pyridyl ketone in aqueous solution. The centrosymmetric complex cation is structurally similar to that found in previously reported salts and exhibits Cu—O bonds deviating by 25 degrees from an octahedral geometry by the so-called ‘off-axis angle’ distortion. The BF4 − anion exhibits a two site disorder of the fluorine atoms [ratio 0.210 (8):0.790 (8)].
Related literature
For related structures, see: Wang et al. (1986 ▶); Tangoulis et al. (1997 ▶); Yang et al. (1998 ▶); Tong et al. (1998 ▶); Serna et al. (1999 ▶); Reinoso et al. (2003 ▶); Li et al. (2005 ▶).
Experimental
Crystal data
[Cu(C11H10N2O2)2](BF4)2·2H2O
M r = 677.61
Monoclinic,
a = 7.8147 (2) Å
b = 14.4225 (4) Å
c = 12.1840 (3) Å
β = 101.160 (3)°
V = 1347.26 (6) Å3
Z = 2
Mo Kα radiation
μ = 0.91 mm−1
T = 293 K
0.8 × 0.6 × 0.6 mm
Data collection
Oxford Diffraction Sapphire CCD diffractometer
Absorption correction: multi-scan SCALE3 ABSPACK in CrysAlis RED (Oxford Diffraction, 2006 ▶) T min = 0.474, T max = 0.579
25175 measured reflections
5349 independent reflections
4145 reflections with I > 2σ(I)
R int = 0.036
Refinement
R[F 2 > 2σ(F 2)] = 0.055
wR(F 2) = 0.192
S = 1.21
5349 reflections
219 parameters
10 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.72 e Å−3
Δρmin = −1.03 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2006 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2006 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809016973/fj2210sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809016973/fj2210Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| Cu1—N1i | 2.0099 (19) |
| Cu1—N1 | 2.0099 (19) |
| Cu1—N2 | 2.0146 (19) |
| Cu1—N2i | 2.0147 (19) |
| Cu1—O1 | 2.4312 (17) |
| Cu1—O1i | 2.4312 (17) |
Symmetry code: (i)
.
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O2—H2⋯O3 | 0.82 | 1.87 | 2.686 (3) | 172 |
Symmetry codes: .
Acknowledgments
The diffractometer was purchased with funding from the National Science Foundation (NSF # 0420322). Additional funding is from a CSUAAUP research grant.
supplementary crystallographic information
Experimental
All chemicals and reagents were purchased from Aldrich and used as received. di-2-pyridyl ketone (2 mmol) and copper(II) tetrafluorborate hexahydrate (1 mmol) were combined in 40 ml of water and stirred for 30 minutes. The resulting violet crystals were isolated after 48 h by slow evaporation of the solution.
Refinement
For structure solution, direct methods were used to locate the initial structural model that consisted of all non-hydrogen atoms. All ligand-based H atoms were added during the refinement stage at idealized positions. Water-based H atoms were found during subsequent cycles from difference maps and their bond lengths to oxygen were free to refine. All H atoms were refined isotropically and all non-hydrogen atoms were refined anisotropically.
Figures
Fig. 1.
ORTEP representation of the title complex. Thermal ellipsoids are drawn at the 30% probability level and H atoms have been omitted for clarity.
Crystal data
| [Cu(C11H10N2O2)2](BF4)2·2H2O | F(000) = 686 |
| Mr = 677.61 | Dx = 1.670 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 5349 reflections |
| a = 7.8147 (2) Å | θ = 3.8–32.0° |
| b = 14.4225 (4) Å | µ = 0.91 mm−1 |
| c = 12.1840 (3) Å | T = 293 K |
| β = 101.160 (3)° | Parallelpiped, violet |
| V = 1347.26 (6) Å3 | 0.8 × 0.6 × 0.6 mm |
| Z = 2 |
Data collection
| Oxford Diffraction Sapphire CCD diffractometer | 5349 independent reflections |
| Radiation source: fine-focus sealed tube | 4145 reflections with I > 2σ(I) |
| graphite | Rint = 0.036 |
| ω scans | θmax = 34.7°, θmin = 3.9° |
| Absorption correction: multi-scan SCALE3 ABSPACK in CrysAlis RED (Oxford Diffraction, 2006) | h = −12→11 |
| Tmin = 0.474, Tmax = 0.579 | k = −22→22 |
| 25175 measured reflections | l = −18→19 |
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)] = 0.055 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.192 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.21 | w = 1/[σ^2^(Fo^2^) + (0.0959P)^2^ + 1.P] where P = (Fo^2^ + 2Fc^2^)/3 |
| 5349 reflections | (Δ/σ)max < 0.001 |
| 219 parameters | Δρmax = 0.72 e Å−3 |
| 10 restraints | Δρmin = −1.03 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. Hydrogen atoms were included in calculated positions for the ring carbons on the dpk ligand (0.93Å for sp2 carbons) and were included in the refinement in riding motion approximation with Uiso = 1.2Ueq of the carrier atom for sp2 carbons. Oxygen hydrogens were found in difference maps.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 | Occ. (<1) | |
| Cu1 | 0.0000 | 0.0000 | 0.5000 | 0.02185 (12) | |
| C1 | 0.2975 (3) | 0.04790 (18) | 0.3891 (2) | 0.0289 (5) | |
| H1 | 0.2514 | 0.0035 | 0.3363 | 0.035* | |
| C2 | 0.4472 (4) | 0.0936 (2) | 0.3777 (2) | 0.0335 (5) | |
| H2A | 0.5001 | 0.0810 | 0.3172 | 0.040* | |
| C3 | 0.5190 (4) | 0.1586 (2) | 0.4571 (2) | 0.0348 (5) | |
| H3 | 0.6217 | 0.1894 | 0.4517 | 0.042* | |
| C4 | 0.4334 (3) | 0.17694 (18) | 0.5455 (2) | 0.0310 (5) | |
| H4 | 0.4780 | 0.2203 | 0.6001 | 0.037* | |
| C5 | 0.2824 (3) | 0.12975 (15) | 0.55022 (18) | 0.0243 (4) | |
| C6 | 0.1798 (3) | 0.14291 (15) | 0.64412 (18) | 0.0240 (4) | |
| C7 | 0.1983 (3) | 0.05478 (15) | 0.71483 (18) | 0.0228 (4) | |
| C8 | 0.2869 (4) | 0.05111 (17) | 0.8236 (2) | 0.0294 (5) | |
| H8 | 0.3411 | 0.1036 | 0.8587 | 0.035* | |
| C9 | 0.2936 (4) | −0.03360 (19) | 0.8802 (2) | 0.0322 (5) | |
| H9 | 0.3511 | −0.0383 | 0.9543 | 0.039* | |
| C10 | 0.2138 (4) | −0.11005 (17) | 0.8244 (2) | 0.0289 (4) | |
| H10 | 0.2176 | −0.1671 | 0.8604 | 0.035* | |
| C11 | 0.1283 (3) | −0.10113 (16) | 0.71447 (19) | 0.0250 (4) | |
| H11 | 0.0746 | −0.1529 | 0.6772 | 0.030* | |
| N1 | 0.2158 (3) | 0.06543 (13) | 0.47416 (15) | 0.0230 (3) | |
| N2 | 0.1204 (3) | −0.02000 (13) | 0.65999 (15) | 0.0214 (3) | |
| O1 | 0.0028 (2) | 0.15157 (12) | 0.58765 (14) | 0.0252 (3) | |
| O2 | 0.2355 (3) | 0.21705 (12) | 0.71285 (15) | 0.0310 (4) | |
| H2 | 0.2214 | 0.2651 | 0.6763 | 0.047* | |
| H50 | −0.064 (5) | 0.153 (3) | 0.633 (3) | 0.034 (9)* | |
| H51 | 0.181 (7) | 0.416 (4) | 0.599 (4) | 0.058 (13)* | |
| H52 | 0.133 (6) | 0.354 (3) | 0.529 (4) | 0.044 (11)* | |
| O3 | 0.2110 (4) | 0.36785 (16) | 0.5814 (2) | 0.0419 (5) | |
| B1 | 0.8127 (4) | 0.13674 (19) | 0.8480 (2) | 0.0302 (5) | 0.790 (8) |
| F1 | 0.7868 (2) | 0.16783 (13) | 0.73741 (13) | 0.0381 (4) | 0.790 (8) |
| F2 | 0.8638 (9) | 0.0451 (3) | 0.8536 (8) | 0.0471 (13) | 0.790 (8) |
| F3 | 0.9557 (7) | 0.1892 (2) | 0.9056 (3) | 0.0674 (14) | 0.790 (8) |
| F4 | 0.6729 (5) | 0.1531 (3) | 0.8951 (3) | 0.0661 (12) | 0.790 (8) |
| B1B | 0.8127 (4) | 0.13674 (19) | 0.8480 (2) | 0.0302 (5) | 0.210 (8) |
| F1B | 0.7868 (2) | 0.16783 (13) | 0.73741 (13) | 0.0381 (4) | 0.210 (8) |
| F2B | 0.894 (4) | 0.0519 (14) | 0.854 (3) | 0.0471 (13) | 0.210 (8) |
| F3B | 0.866 (3) | 0.1927 (9) | 0.9307 (11) | 0.0674 (14) | 0.210 (8) |
| F4B | 0.6394 (16) | 0.1147 (11) | 0.8558 (12) | 0.0661 (12) | 0.210 (8) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.0261 (2) | 0.02088 (19) | 0.01787 (18) | −0.00313 (13) | 0.00248 (13) | −0.00088 (12) |
| C1 | 0.0302 (11) | 0.0331 (12) | 0.0238 (10) | −0.0027 (9) | 0.0066 (8) | 0.0000 (8) |
| C2 | 0.0302 (12) | 0.0398 (14) | 0.0323 (12) | −0.0002 (10) | 0.0109 (9) | 0.0049 (10) |
| C3 | 0.0271 (12) | 0.0358 (13) | 0.0423 (14) | −0.0049 (9) | 0.0088 (10) | 0.0050 (11) |
| C4 | 0.0308 (12) | 0.0257 (10) | 0.0350 (12) | −0.0068 (9) | 0.0024 (9) | 0.0008 (9) |
| C5 | 0.0271 (10) | 0.0209 (9) | 0.0234 (9) | −0.0013 (7) | 0.0016 (7) | 0.0019 (7) |
| C6 | 0.0313 (11) | 0.0184 (8) | 0.0210 (9) | −0.0036 (7) | 0.0016 (7) | −0.0010 (7) |
| C7 | 0.0248 (10) | 0.0206 (9) | 0.0223 (9) | −0.0026 (7) | 0.0030 (7) | −0.0012 (7) |
| C8 | 0.0352 (12) | 0.0263 (10) | 0.0246 (10) | −0.0040 (9) | 0.0006 (8) | −0.0005 (8) |
| C9 | 0.0397 (13) | 0.0323 (12) | 0.0222 (10) | −0.0016 (10) | 0.0004 (9) | 0.0025 (9) |
| C10 | 0.0351 (12) | 0.0249 (10) | 0.0259 (10) | −0.0006 (9) | 0.0037 (9) | 0.0046 (8) |
| C11 | 0.0259 (10) | 0.0206 (9) | 0.0285 (10) | −0.0024 (7) | 0.0053 (8) | 0.0008 (7) |
| N1 | 0.0239 (8) | 0.0236 (8) | 0.0213 (8) | −0.0030 (6) | 0.0036 (6) | 0.0005 (6) |
| N2 | 0.0241 (8) | 0.0198 (7) | 0.0201 (7) | −0.0016 (6) | 0.0035 (6) | −0.0003 (6) |
| O1 | 0.0270 (8) | 0.0252 (7) | 0.0227 (7) | 0.0009 (6) | 0.0026 (6) | 0.0011 (6) |
| O2 | 0.0455 (11) | 0.0198 (7) | 0.0257 (8) | −0.0050 (7) | 0.0019 (7) | −0.0033 (6) |
| O3 | 0.0584 (14) | 0.0259 (9) | 0.0390 (11) | 0.0041 (9) | 0.0035 (10) | 0.0029 (8) |
| B1 | 0.0412 (15) | 0.0245 (11) | 0.0250 (11) | 0.0042 (10) | 0.0064 (10) | 0.0002 (9) |
| F1 | 0.0457 (10) | 0.0417 (9) | 0.0268 (7) | 0.0064 (7) | 0.0072 (6) | 0.0068 (6) |
| F2 | 0.069 (3) | 0.0238 (11) | 0.0477 (10) | 0.0088 (16) | 0.010 (2) | 0.0005 (10) |
| F3 | 0.094 (3) | 0.0412 (13) | 0.0503 (17) | −0.0201 (19) | −0.0284 (19) | 0.0030 (12) |
| F4 | 0.084 (2) | 0.072 (3) | 0.054 (2) | 0.0369 (19) | 0.0436 (18) | 0.0173 (17) |
| B1B | 0.0412 (15) | 0.0245 (11) | 0.0250 (11) | 0.0042 (10) | 0.0064 (10) | 0.0002 (9) |
| F1B | 0.0457 (10) | 0.0417 (9) | 0.0268 (7) | 0.0064 (7) | 0.0072 (6) | 0.0068 (6) |
| F2B | 0.069 (3) | 0.0238 (11) | 0.0477 (10) | 0.0088 (16) | 0.010 (2) | 0.0005 (10) |
| F3B | 0.094 (3) | 0.0412 (13) | 0.0503 (17) | −0.0201 (19) | −0.0284 (19) | 0.0030 (12) |
| F4B | 0.084 (2) | 0.072 (3) | 0.054 (2) | 0.0369 (19) | 0.0436 (18) | 0.0173 (17) |
Geometric parameters (Å, °)
| Cu1—N1i | 2.0099 (19) | C6—C7 | 1.527 (3) |
| Cu1—N1 | 2.0099 (19) | C7—N2 | 1.350 (3) |
| Cu1—N2 | 2.0146 (19) | C7—C8 | 1.372 (3) |
| Cu1—N2i | 2.0147 (19) | C8—C9 | 1.399 (4) |
| Cu1—O1 | 2.4312 (17) | C8—H8 | 0.9300 |
| Cu1—O1i | 2.4312 (17) | C9—C10 | 1.379 (4) |
| C1—N1 | 1.343 (3) | C9—H9 | 0.9300 |
| C1—C2 | 1.373 (4) | C10—C11 | 1.382 (3) |
| C1—H1 | 0.9300 | C10—H10 | 0.9300 |
| C2—C3 | 1.385 (4) | C11—N2 | 1.341 (3) |
| C2—H2A | 0.9300 | C11—H11 | 0.9300 |
| C3—C4 | 1.399 (4) | O1—H50 | 0.83 (4) |
| C3—H3 | 0.9300 | O2—H2 | 0.8200 |
| C4—C5 | 1.373 (3) | O3—H51 | 0.78 (5) |
| C4—H4 | 0.9300 | O3—H52 | 0.82 (5) |
| C5—N1 | 1.343 (3) | B1—F4 | 1.350 (4) |
| C5—C6 | 1.531 (3) | B1—F2 | 1.378 (5) |
| C6—O2 | 1.376 (3) | B1—F1 | 1.397 (3) |
| C6—O1 | 1.427 (3) | B1—F3 | 1.417 (5) |
| N1i—Cu1—N1 | 179.999 (1) | O1—C6—C5 | 104.48 (17) |
| N1i—Cu1—N2 | 91.74 (8) | C7—C6—C5 | 108.21 (18) |
| N1—Cu1—N2 | 88.27 (8) | N2—C7—C8 | 122.8 (2) |
| N1i—Cu1—N2i | 88.26 (8) | N2—C7—C6 | 113.67 (19) |
| N1—Cu1—N2i | 91.73 (8) | C8—C7—C6 | 123.5 (2) |
| N2—Cu1—N2i | 180.0 | C7—C8—C9 | 118.3 (2) |
| N1i—Cu1—O1 | 106.84 (7) | C7—C8—H8 | 120.9 |
| N1—Cu1—O1 | 73.16 (7) | C9—C8—H8 | 120.9 |
| N2—Cu1—O1 | 74.99 (7) | C10—C9—C8 | 119.0 (2) |
| N2i—Cu1—O1 | 105.01 (7) | C10—C9—H9 | 120.5 |
| N1i—Cu1—O1i | 73.16 (7) | C8—C9—H9 | 120.5 |
| N1—Cu1—O1i | 106.84 (7) | C11—C10—C9 | 119.4 (2) |
| N2—Cu1—O1i | 105.01 (7) | C11—C10—H10 | 120.3 |
| N2i—Cu1—O1i | 74.99 (7) | C9—C10—H10 | 120.3 |
| O1—Cu1—O1i | 180.00 (8) | N2—C11—C10 | 121.9 (2) |
| N1—C1—C2 | 122.0 (2) | N2—C11—H11 | 119.1 |
| N1—C1—H1 | 119.0 | C10—C11—H11 | 119.1 |
| C2—C1—H1 | 119.0 | C5—N1—C1 | 118.9 (2) |
| C1—C2—C3 | 119.5 (2) | C5—N1—Cu1 | 116.18 (15) |
| C1—C2—H2A | 120.2 | C1—N1—Cu1 | 124.86 (16) |
| C3—C2—H2A | 120.2 | C11—N2—C7 | 118.63 (19) |
| C2—C3—C4 | 118.4 (2) | C11—N2—Cu1 | 124.89 (15) |
| C2—C3—H3 | 120.8 | C7—N2—Cu1 | 116.48 (15) |
| C4—C3—H3 | 120.8 | C6—O1—Cu1 | 93.35 (12) |
| C5—C4—C3 | 118.8 (2) | C6—O1—H50 | 111 (3) |
| C5—C4—H4 | 120.6 | Cu1—O1—H50 | 111 (3) |
| C3—C4—H4 | 120.6 | C6—O2—H2 | 109.5 |
| N1—C5—C4 | 122.3 (2) | H51—O3—H52 | 103 (5) |
| N1—C5—C6 | 114.34 (19) | F4—B1—F2 | 113.4 (4) |
| C4—C5—C6 | 123.3 (2) | F4—B1—F1 | 112.1 (3) |
| O2—C6—O1 | 112.86 (19) | F2—B1—F1 | 110.0 (4) |
| O2—C6—C7 | 108.62 (18) | F4—B1—F3 | 108.8 (3) |
| O1—C6—C7 | 108.78 (18) | F2—B1—F3 | 107.1 (4) |
| O2—C6—C5 | 113.67 (19) | F1—B1—F3 | 105.0 (3) |
Symmetry codes: (i) −x, −y, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O2—H2···O3 | 0.82 | 1.87 | 2.686 (3) | 172 |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2210).
References
- Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
- Li, C.-J., Li, W., Tong, M.-L. & Ng, S. W. (2005). Acta Cryst. E61, m232–m234.
- Oxford Diffraction (2006). CrysAlis CCD and CrysAlis RED Oxford Diffraction, Abingdon, England.
- Reinoso, S., Vitoria, P., San Felices, L., Lezama, L. & Gutiérrez-Zorrilla, J. M. (2003). Acta Cryst. E59, m548–m550.
- Serna, Z., Barandika, M. G., Cortés, R., Urtiaga, M. K. & Arriortua, M. I. (1999). Polyhedron, 18, 249–255.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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- Tong, M.-L., Yang, G., Chen, X.-M. & Ng, S. W. (1998). Acta Cryst. C54, 217–219.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809016973/fj2210sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809016973/fj2210Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

