The title compound, [Cu(CHO
2)
2(C
6H
12N
2)(H
2O)]
n, forms a polymeric chain, [Cu(HCOO)
2(dabco)(H
2O)]
∞ (dabco is 1,4-diazabicyclo[2.2.2]octane). Both formate ligands are O-monodentate anions and dabco acts as a bridging ligand, creating a linear polymeric arrangement interconnected by O
water—H
O
carboxy hydrogen bonds. The deformed square-pyramidal Cu
II coordination comprises two N and two O atoms as the base, and a water molecule in the apical position. The point symmetry of the Cu
II polyhedron and the dabco ligand is
mm, and the formate anions lie on the mirror planes ¼,
y, z and ¾,
y, z.
Supporting information
CCDC reference: 222826
Key indicators
- Single-crystal X-ray study
- T = 293 K
- Mean (C-C) = 0.003 Å
- R factor = 0.023
- wR factor = 0.062
- Data-to-parameter ratio = 10.9
checkCIF/PLATON results
No syntax errors found
Alert level C
CRYSC01_ALERT_1_C The word below has not been recognised as a standard
identifier.
turquoise
CRYSC01_ALERT_1_C No recognised colour has been given for crystal colour.
PLAT164_ALERT_4_C Nr. of Refined C-H H-Atoms in Heavy-At Struct... 4
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
3 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 ALERT type 2 Indicator that the structure model may be wrong or deficient
0 ALERT type 3 Indicator that the structure quality may be low
1 ALERT type 4 Improvement, methodology, query or suggestion
The title complex was prepared by dissolving cupric formate [2 mmol, Cu(HCOO)2·2H2O] in 50 ml of water with dabco (2 mmol, C6H12N2). After heating to boiling, a few drops of formic acid were added to clear the solution. The solution was filtered and allowed to cool. After several days, turquoise crystals were obtained.
All H atoms were located from a difference synthesis and refined isotropically.
Data collection: P3 (Siemens, 1993); cell refinement: P3; data reduction: XDISK in SHELXTL/PC (Sheldrick, 1990); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997b); molecular graphics: XP in SHELXTL/PC; software used to prepare material for publication: PLATON (Spek, 1990).
catena-Poly[[aqua(diformato-
κO)copper(II)]-µ-1,4-diazabicyclo[2.2.2]octane-
κ2N:
N']
top
Crystal data top
[Cu(CHO2)2(C6H12N2)(H2O)] | F(000) = 294 |
Mr = 283.77 | Dx = 1.786 Mg m−3 |
Orthorhombic, Pmmn | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ab 2a | Cell parameters from 38 reflections |
a = 6.8084 (13) Å | θ = 5–18° |
b = 12.071 (2) Å | µ = 2.08 mm−1 |
c = 6.4224 (15) Å | T = 293 K |
V = 527.80 (19) Å3 | Prism, turquoise |
Z = 2 | 0.30 × 0.20 × 0.20 mm |
Data collection top
Siemens P3 diffractometer | 710 reflections with I > 2σ(I) |
Radiation source: FK60-10 Siemens Mo tube | Rint = 0.000 |
Graphite monochromator | θmax = 28.0°, θmin = 3.2° |
ω–2θ scans | h = 0→8 |
Absorption correction: psi scan (North et al., 1968) | k = 0→15 |
Tmin = 0.557, Tmax = 0.661 | l = 0→8 |
719 measured reflections | 3 standard reflections every 100 reflections |
719 independent reflections | intensity decay: none |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: structure-invariant direct methods |
R[F2 > 2σ(F2)] = 0.023 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.062 | All H-atom parameters refined |
S = 1.23 | w = 1/[σ2(Fo2) + (0.0345P)2 + 0.21P] where P = (Fo2 + 2Fc2)/3 |
719 reflections | (Δ/σ)max < 0.001 |
66 parameters | Δρmax = 0.39 e Å−3 |
0 restraints | Δρmin = −0.49 e Å−3 |
0 constraints | |
Crystal data top
[Cu(CHO2)2(C6H12N2)(H2O)] | V = 527.80 (19) Å3 |
Mr = 283.77 | Z = 2 |
Orthorhombic, Pmmn | Mo Kα radiation |
a = 6.8084 (13) Å | µ = 2.08 mm−1 |
b = 12.071 (2) Å | T = 293 K |
c = 6.4224 (15) Å | 0.30 × 0.20 × 0.20 mm |
Data collection top
Siemens P3 diffractometer | 710 reflections with I > 2σ(I) |
Absorption correction: psi scan (North et al., 1968) | Rint = 0.000 |
Tmin = 0.557, Tmax = 0.661 | 3 standard reflections every 100 reflections |
719 measured reflections | intensity decay: none |
719 independent reflections | |
Refinement top
R[F2 > 2σ(F2)] = 0.023 | 0 restraints |
wR(F2) = 0.062 | All H-atom parameters refined |
S = 1.23 | Δρmax = 0.39 e Å−3 |
719 reflections | Δρmin = −0.49 e Å−3 |
66 parameters | |
Special details top
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All e.s.d.'s are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 | |
Cu | 0.25 | 0.25 | 0.33505 (5) | 0.0180 (1) | |
O1 | 0.25 | 0.25 | 0.6835 (4) | 0.0341 (8) | |
O2 | 0.25 | 0.08926 (14) | 0.2903 (3) | 0.0290 (4) | |
O3 | 0.25 | 0.0745 (2) | −0.0562 (4) | 0.0630 (8) | |
N1 | 0.5573 (3) | 0.25 | 0.3413 (3) | 0.0197 (4) | |
C2 | 0.25 | 0.03800 (19) | 0.1200 (4) | 0.0315 (7) | |
C3 | 0.6379 (3) | 0.25 | 0.1269 (4) | 0.0299 (7) | |
C4 | 0.6384 (2) | 0.15119 (16) | 0.4490 (3) | 0.0360 (5) | |
H1 | 0.25 | 0.316 (3) | 0.761 (8) | 0.074 (13)* | |
H2 | 0.25 | −0.041 (3) | 0.139 (5) | 0.039 (9)* | |
H3 | 0.588 (4) | 0.313 (2) | 0.068 (5) | 0.054 (7)* | |
H4A | 0.585 (5) | 0.089 (3) | 0.385 (5) | 0.083 (11)* | |
H4B | 0.580 (5) | 0.154 (3) | 0.591 (6) | 0.079 (10)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cu | 0.0165 (2) | 0.0164 (2) | 0.0212 (2) | 0 | 0 | 0 |
O1 | 0.0450 (15) | 0.0361 (14) | 0.0211 (11) | 0 | 0 | 0 |
O2 | 0.0275 (8) | 0.0212 (7) | 0.0382 (8) | 0 | 0 | −0.0071 (7) |
O3 | 0.109 (2) | 0.0426 (12) | 0.0373 (10) | 0 | 0 | 0.0064 (10) |
N1 | 0.0180 (7) | 0.0182 (8) | 0.0229 (8) | 0 | −0.0003 (6) | 0 |
C2 | 0.0381 (13) | 0.0194 (10) | 0.0370 (11) | 0 | 0 | −0.0021 (9) |
C3 | 0.0217 (11) | 0.0467 (14) | 0.0212 (9) | 0 | −0.0009 (8) | 0 |
C4 | 0.0206 (8) | 0.0337 (9) | 0.0537 (10) | −0.0016 (7) | −0.0027 (7) | 0.0226 (8) |
Geometric parameters (Å, º) top
Cu—O1 | 2.238 (2) | N1—C4 | 1.485 (2) |
Cu—O2 | 1.962 (2) | C3—C3i | 1.526 (4) |
Cu—N1 | 2.093 (2) | C4—C4ii | 1.520 (3) |
O2—C2 | 1.257 (3) | C2—H2 | 0.97 (3) |
O3—C2 | 1.214 (4) | C3—H3 | 0.92 (3) |
O1—H1 | 0.94 (4) | C4—H4A | 0.93 (4) |
N1—C3 | 1.482 (3) | C4—H4B | 1.00 (4) |
| | | |
O1—Cu—O2 | 98.42 (6) | N1—C3—C3i | 111.7 (2) |
O1—Cu—N1 | 88.90 (5) | N1—C4—C4ii | 111.82 (15) |
O2—Cu—N1 | 90.16 (1) | O2—C2—H2 | 112.2 (19) |
O2—Cu—O2iii | 163.16 (11) | O3—C2—H2 | 118.6 (19) |
N1—Cu—N1iii | 177.81 (9) | N1—C3—H3 | 104 (2) |
Cu—O2—C2 | 127.92 (16) | C3i—C3—H3 | 111.8 (17) |
H1—O1—H1iii | 116 (4) | H3—C3—H3iv | 112 (3) |
Cu—O1—H1 | 122 (3) | N1—C4—H4A | 107 (2) |
Cu—N1—C3 | 110.63 (14) | N1—C4—H4B | 105 (2) |
Cu—N1—C4 | 112.37 (10) | H4A—C4—H4B | 106 (3) |
C4—N1—C4iv | 106.85 (16) | C4ii—C4—H4A | 113 (2) |
C3—N1—C4 | 107.16 (12) | C4ii—C4—H4B | 114 (2) |
O2—C2—O3 | 129.2 (2) | | |
| | | |
N1—Cu—O2—C2 | −91.09 (5) | O2—Cu—N1—C4 | −38.15 (13) |
O1—Cu—N1—C4 | 60.28 (12) | Cu—N1—C4—C4ii | 178.97 (12) |
O2—Cu—N1—C3 | 81.58 (6) | C3—N1—C4—C4ii | 57.25 (19) |
Symmetry codes: (i) −x+3/2, −y+1/2, z; (ii) −x+3/2, y, z; (iii) −x+1/2, −y+1/2, z; (iv) x, −y+1/2, z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O3v | 0.94 (4) | 1.77 (4) | 2.699 (3) | 170 (4) |
Symmetry code: (v) −x+1/2, −y+1/2, z+1. |
Experimental details
Crystal data |
Chemical formula | [Cu(CHO2)2(C6H12N2)(H2O)] |
Mr | 283.77 |
Crystal system, space group | Orthorhombic, Pmmn |
Temperature (K) | 293 |
a, b, c (Å) | 6.8084 (13), 12.071 (2), 6.4224 (15) |
V (Å3) | 527.80 (19) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 2.08 |
Crystal size (mm) | 0.30 × 0.20 × 0.20 |
|
Data collection |
Diffractometer | Siemens P3 diffractometer |
Absorption correction | Psi scan (North et al., 1968) |
Tmin, Tmax | 0.557, 0.661 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 719, 719, 710 |
Rint | 0.000 |
(sin θ/λ)max (Å−1) | 0.661 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.023, 0.062, 1.23 |
No. of reflections | 719 |
No. of parameters | 66 |
H-atom treatment | All H-atom parameters refined |
Δρmax, Δρmin (e Å−3) | 0.39, −0.49 |
Selected geometric parameters (Å, º) topCu—O1 | 2.238 (2) | O2—C2 | 1.257 (3) |
Cu—O2 | 1.962 (2) | O3—C2 | 1.214 (4) |
Cu—N1 | 2.093 (2) | | |
| | | |
O1—Cu—O2 | 98.42 (6) | O2—Cu—O2i | 163.16 (11) |
O1—Cu—N1 | 88.90 (5) | N1—Cu—N1i | 177.81 (9) |
O2—Cu—N1 | 90.16 (1) | | |
Symmetry code: (i) −x+1/2, −y+1/2, z. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O3ii | 0.94 (4) | 1.77 (4) | 2.699 (3) | 170 (4) |
Symmetry code: (ii) −x+1/2, −y+1/2, z+1. |
So far, CuII–dabco coordination has not been intensively investigated. Only one mononuclear structure (Karan et al., 1999), two dinuclear structures (Durley et al., 1980; Maverick et al., 1986) and one polymeric structure (Rao et al., 1983) of CuII compounds containing the dabco ligand have been reported. The present paper reports the first example of the coordination of the dabco ligand in an equatorial position of a square-pyramidal CuII polyhedron. The structure of the title complex, (I), is polymeric with [Cu(HCOO)2(dabco)(H2O)]∞ chains running along the a axis. Fig. 1 shows the independent fragment of the chain.
The chain consists of pentacoordinated CuII ions in a distorted square-pyramidal (SQP) geometry, with two Cu—N bonds of 2.093 (2) Å and two Cu—O bonds of 1.962 (2) Å of the formate groups in the basal plane. The apical position is occupied by the water molecule [Cu—OH2 = 2.238 (2) Å]. The Cu atom is displaced from the basal plane by 0.124 (1) Å towards atom O1. The point symmetry of the CuII polyhedron and the dabco ligand is mm, and the formate anions lie on the mirror planes 1/4,y,z and 3/4,y,z.
The observed SQP coordination is distinctly deformed in the direction of trigonal-bipiramidal (TBP) coordination, with the trigonality parameter τ = 0.24 [τ is defined by Addison et al. (1984); for a regular SQP structure, the trigonality parameter is 0, and for TBP distortion it increases to 1].
The formate group acts as a monodentate ligand, the distance between the CuII ion and uncoordinated atom O3 is 3.287 (3) Å. Such behaviour may be caused by the participation of this atom in a strong hydrogen bond with the water molecule. These interchain interactions, running along the z axis, are shown in Fig. 2. This strong hydrogen bond does not cause a delocalization of the π bond in the carboxyl group. The C2—O2 and C2—O3 bonds are distinctly different [1.257 (3) and 1.214 (4) Å, respectively].
The intrachain Cu···Cu distance of 6.808 (1) Å is longer than the shortest interchain Cu···Cu distance of 6.422 (2) Å along the c axis. Another short interchain Cu···Cu distances of 7.246 (2) and 8.157 (2) Å are between the two CuII ions related by the screw axis 21 and with no spacer between them.