supplementary materials
-Succinato-
2O1:O4-bis[(2,2'-bipyridine-
2N,N')copper(II)] succinate dodecahydrate
In the title compound, [Cu2(C4H4O4)(C10H8N2)4]C4H4O4·12H2O, C10H8N2), the centrosymmetic dinuclear cations, succinate anions and water molecules are hydrogen bonded into layers parallel to (010). The Cu atom is square-pyramidally coordinated by one atom of the succinato ligand and four N atoms of two 2,2'-bipyridine ligands. The 12 water molecules form a new type of water cluster.
Addition of 10 ml CH3OH containing 0.324 g (2.08 mmol) 2,2'-bipyridine (bpy)
to an aqueous solution of 0.171 g (1.00 mmol) CuCl2.2H2O in 10 ml H2O
gave a blue solution, then added 0.182 g (1.00 mmol) succinic acid to the
mixture. The mixture was further stirred vigorously, and the resulting blue
solution was adjusted with NaOH to pH = 8.3 and allowed to stand at room
temperature. After two weeks, a small amount of blue block crystals had grown.
H atoms bonded to C atoms were palced in geometrically calculated position and
were refined using a riding model, with Uiso(H) = 1.2
Ueq(C). H atoms attached to O atoms were found in a difference
Fourier synthesis and were refined using a riding model.
Data collection: XSCANS (Siemens, 1996); cell refinement: XSCANS (Siemens, 1996); data reduction: XSCANS (Siemens, 1996); 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 (Sheldrick, 2008).
µ-Succinato-
κ2O1:
O4-bis[(2,2'-bipyridine-
κ2N,
N')copper(II)] succinate dodecahydrate
top
Crystal data top
| [Cu2(C4H4O4)(C10H8N2)4]C4H4O4·12H2O | Z = 1 |
| Mr = 1200.15 | F(000) = 626 |
| Triclinic, P1 | Dx = 1.447 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 10.502 (2) Å | Cell parameters from 25 reflections |
| b = 10.764 (2) Å | θ = 5.0–12.5° |
| c = 12.892 (3) Å | µ = 0.85 mm−1 |
| α = 77.21 (3)° | T = 295 K |
| β = 77.99 (3)° | Block, blue |
| γ = 79.85 (3)° | 0.34 × 0.27 × 0.19 mm |
| V = 1377.1 (5) Å3 | |
Data collection top
Bruker P4 diffractometer | 3856 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.025 |
| graphite | θmax = 25.0°, θmin = 1.7° |
| θ/2θ scans | h = −1→12 |
Absorption correction: ψ scan XSCANS | k = −12→12 |
| Tmin = 0.750, Tmax = 0.844 | l = −15→15 |
| 5721 measured reflections | 3 standard reflections every 97 reflections |
| 4853 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: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.053 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.145 | H-atom parameters constrained |
| S = 1.07 | w = 1/[σ2(Fo2) + (0.0531P)2 + 2.9966P] where P = (Fo2 + 2Fc2)/3 |
| 4853 reflections | (Δ/σ)max = 0.001 |
| 353 parameters | Δρmax = 1.03 e Å−3 |
| 18 restraints | Δρmin = −1.58 e Å−3 |
Crystal data top
| [Cu2(C4H4O4)(C10H8N2)4]C4H4O4·12H2O | γ = 79.85 (3)° |
| Mr = 1200.15 | V = 1377.1 (5) Å3 |
| Triclinic, P1 | Z = 1 |
| a = 10.502 (2) Å | Mo Kα radiation |
| b = 10.764 (2) Å | µ = 0.85 mm−1 |
| c = 12.892 (3) Å | T = 295 K |
| α = 77.21 (3)° | 0.34 × 0.27 × 0.19 mm |
| β = 77.99 (3)° | |
Data collection top
Bruker P4 diffractometer | 3856 reflections with I > 2σ(I) |
Absorption correction: ψ scan XSCANS | Rint = 0.025 |
| Tmin = 0.750, Tmax = 0.844 | θmax = 25.0° |
| 5721 measured reflections | 3 standard reflections every 97 reflections |
| 4853 independent reflections | intensity decay: none |
Refinement top
| R[F2 > 2σ(F2)] = 0.053 | H-atom parameters constrained |
| wR(F2) = 0.145 | Δρmax = 1.03 e Å−3 |
| S = 1.07 | Δρmin = −1.58 e Å−3 |
| 4853 reflections | Absolute structure: ? |
| 353 parameters | Flack parameter: ? |
| 18 restraints | Rogers parameter: ? |
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 | |
| Cu1 | 0.74197 (5) | 0.97679 (5) | 0.74602 (4) | 0.03307 (17) | |
| N1 | 0.7538 (3) | 1.0058 (3) | 0.8941 (3) | 0.0375 (8) | |
| N2 | 0.6286 (4) | 0.8488 (3) | 0.8385 (3) | 0.0393 (8) | |
| N3 | 0.9308 (3) | 0.8594 (3) | 0.7123 (3) | 0.0385 (8) | |
| N4 | 0.8548 (3) | 1.1107 (3) | 0.6606 (2) | 0.0328 (7) | |
| O1 | 0.6673 (3) | 0.9791 (3) | 0.6165 (2) | 0.0370 (7) | |
| O2 | 0.5113 (3) | 1.1205 (3) | 0.6850 (2) | 0.0479 (8) | |
| O3 | 0.3066 (4) | 0.3885 (4) | 0.4609 (3) | 0.0632 (10) | |
| O4 | 0.4199 (4) | 0.4917 (4) | 0.3143 (3) | 0.0719 (11) | |
| O5 | 0.7964 (4) | 0.5153 (5) | 0.0060 (3) | 0.0875 (14) | |
| O6 | 0.9811 (4) | 0.6789 (4) | −0.0001 (3) | 0.0816 (12) | |
| O7 | 0.0176 (4) | 0.3001 (5) | 0.7912 (3) | 0.0787 (12) | |
| O8 | 0.2760 (3) | 0.2866 (3) | 0.6727 (3) | 0.0581 (9) | |
| O9 | 0.6523 (4) | 0.5599 (4) | 0.2004 (3) | 0.0639 (10) | |
| O10 | 0.2260 (5) | 0.5285 (5) | 0.1913 (4) | 0.0970 (16) | |
| C1 | 0.8295 (5) | 1.0819 (5) | 0.9166 (4) | 0.0481 (11) | |
| H1A | 0.8774 | 1.1339 | 0.8600 | 0.058* | |
| C2 | 0.8378 (6) | 1.0848 (5) | 1.0216 (4) | 0.0603 (14) | |
| H2A | 0.8915 | 1.1373 | 1.0353 | 0.072* | |
| C3 | 0.7667 (6) | 1.0101 (6) | 1.1047 (4) | 0.0670 (16) | |
| H3A | 0.7710 | 1.0117 | 1.1757 | 0.080* | |
| C4 | 0.6883 (6) | 0.9320 (5) | 1.0835 (4) | 0.0559 (13) | |
| H4A | 0.6389 | 0.8808 | 1.1397 | 0.067* | |
| C5 | 0.6844 (4) | 0.9312 (4) | 0.9766 (3) | 0.0380 (10) | |
| C6 | 0.6070 (4) | 0.8479 (4) | 0.9453 (3) | 0.0385 (10) | |
| C7 | 0.5218 (5) | 0.7736 (5) | 1.0173 (4) | 0.0535 (13) | |
| H7A | 0.5069 | 0.7758 | 1.0905 | 0.064* | |
| C8 | 0.4584 (6) | 0.6953 (5) | 0.9794 (5) | 0.0652 (15) | |
| H8A | 0.3998 | 0.6445 | 1.0267 | 0.078* | |
| C9 | 0.4830 (6) | 0.6936 (5) | 0.8710 (5) | 0.0645 (15) | |
| H9A | 0.4423 | 0.6405 | 0.8441 | 0.077* | |
| C10 | 0.5681 (5) | 0.7709 (5) | 0.8026 (4) | 0.0524 (12) | |
| H10A | 0.5844 | 0.7694 | 0.7291 | 0.063* | |
| C11 | 0.9635 (5) | 0.7332 (5) | 0.7468 (4) | 0.0522 (12) | |
| H11A | 0.8972 | 0.6837 | 0.7815 | 0.063* | |
| C12 | 1.0915 (6) | 0.6737 (5) | 0.7330 (4) | 0.0642 (16) | |
| H12A | 1.1114 | 0.5860 | 0.7585 | 0.077* | |
| C13 | 1.1884 (6) | 0.7463 (6) | 0.6812 (5) | 0.0660 (16) | |
| H13A | 1.2758 | 0.7087 | 0.6721 | 0.079* | |
| C14 | 1.1561 (5) | 0.8762 (5) | 0.6421 (4) | 0.0558 (13) | |
| H14A | 1.2210 | 0.9262 | 0.6046 | 0.067* | |
| C15 | 1.0263 (4) | 0.9304 (4) | 0.6595 (3) | 0.0373 (10) | |
| C16 | 0.9817 (4) | 1.0698 (4) | 0.6231 (3) | 0.0346 (9) | |
| C17 | 1.0628 (4) | 1.1533 (5) | 0.5547 (3) | 0.0443 (11) | |
| H17A | 1.1495 | 1.1236 | 0.5281 | 0.053* | |
| C18 | 1.0132 (5) | 1.2814 (5) | 0.5267 (4) | 0.0517 (12) | |
| H18A | 1.0666 | 1.3389 | 0.4814 | 0.062* | |
| C19 | 0.8851 (5) | 1.3235 (5) | 0.5658 (4) | 0.0494 (12) | |
| H19A | 0.8507 | 1.4096 | 0.5480 | 0.059* | |
| C20 | 0.8082 (5) | 1.2362 (4) | 0.6321 (3) | 0.0420 (10) | |
| H20A | 0.7210 | 1.2646 | 0.6582 | 0.050* | |
| C21 | 0.5588 (4) | 1.0531 (4) | 0.6155 (3) | 0.0334 (9) | |
| C22 | 0.4878 (5) | 1.0601 (4) | 0.5229 (4) | 0.0428 (10) | |
| H22A | 0.3941 | 1.0796 | 0.5479 | 0.051* | |
| H22B | 0.5142 | 1.1306 | 0.4655 | 0.051* | |
| C23 | 0.4059 (5) | 0.4377 (4) | 0.4120 (4) | 0.0452 (11) | |
| C24 | 0.5143 (5) | 0.4410 (4) | 0.4746 (4) | 0.0441 (11) | |
| H24A | 0.5201 | 0.3644 | 0.5306 | 0.053* | |
| H24B | 0.5981 | 0.4415 | 0.4259 | 0.053* | |
| H5B | 0.7666 | 0.4960 | −0.0436 | 0.080* | |
| H5C | 0.7444 | 0.5361 | 0.0614 | 0.079* | |
| H6B | 0.9347 | 0.6242 | −0.0038 | 0.072* | |
| H6C | 1.0555 | 0.6304 | −0.0039 | 0.075* | |
| H7B | 0.0280 | 0.3367 | 0.8405 | 0.071* | |
| H7C | 0.0944 | 0.3014 | 0.7554 | 0.072* | |
| H8B | 0.3482 | 0.2377 | 0.6775 | 0.073* | |
| H8C | 0.2770 | 0.3144 | 0.6058 | 0.060* | |
| H9B | 0.6769 | 0.5981 | 0.2414 | 0.054* | |
| H9C | 0.5793 | 0.5400 | 0.2387 | 0.061* | |
| H10B | 0.1514 | 0.5652 | 0.2154 | 0.092* | |
| H10C | 0.2638 | 0.5022 | 0.2459 | 0.094* | |
Atomic displacement parameters (Å2) top| | U11 | U22 | U33 | U12 | U13 | U23 |
| Cu1 | 0.0336 (3) | 0.0362 (3) | 0.0252 (3) | 0.0014 (2) | −0.00311 (19) | −0.00379 (19) |
| N1 | 0.039 (2) | 0.043 (2) | 0.0283 (17) | 0.0003 (16) | −0.0056 (15) | −0.0060 (15) |
| N2 | 0.041 (2) | 0.0361 (19) | 0.0363 (19) | 0.0005 (16) | −0.0058 (16) | −0.0032 (15) |
| N3 | 0.041 (2) | 0.0392 (19) | 0.0289 (17) | 0.0054 (16) | −0.0042 (15) | −0.0024 (14) |
| N4 | 0.0351 (19) | 0.0361 (18) | 0.0243 (16) | −0.0008 (15) | −0.0037 (14) | −0.0043 (13) |
| O1 | 0.0312 (15) | 0.0495 (17) | 0.0308 (14) | 0.0045 (13) | −0.0103 (12) | −0.0118 (12) |
| O2 | 0.0494 (19) | 0.0567 (19) | 0.0376 (16) | 0.0090 (15) | −0.0112 (14) | −0.0185 (15) |
| O3 | 0.059 (2) | 0.076 (3) | 0.051 (2) | −0.014 (2) | −0.0167 (18) | 0.0055 (18) |
| O4 | 0.068 (3) | 0.111 (3) | 0.0383 (19) | −0.023 (2) | −0.0130 (17) | −0.007 (2) |
| O5 | 0.066 (3) | 0.141 (4) | 0.066 (3) | −0.011 (3) | −0.002 (2) | −0.053 (3) |
| O6 | 0.088 (3) | 0.095 (3) | 0.068 (3) | −0.020 (3) | −0.005 (2) | −0.030 (2) |
| O7 | 0.060 (2) | 0.122 (4) | 0.057 (2) | −0.017 (2) | 0.0023 (19) | −0.032 (2) |
| O8 | 0.048 (2) | 0.073 (2) | 0.0435 (18) | 0.0064 (17) | −0.0043 (15) | −0.0068 (16) |
| O9 | 0.065 (2) | 0.078 (3) | 0.0459 (19) | −0.005 (2) | −0.0001 (17) | −0.0187 (18) |
| O10 | 0.104 (4) | 0.114 (4) | 0.080 (3) | 0.016 (3) | −0.048 (3) | −0.027 (3) |
| C1 | 0.052 (3) | 0.055 (3) | 0.040 (2) | −0.010 (2) | −0.007 (2) | −0.012 (2) |
| C2 | 0.069 (4) | 0.068 (3) | 0.052 (3) | −0.007 (3) | −0.020 (3) | −0.023 (3) |
| C3 | 0.087 (4) | 0.081 (4) | 0.035 (3) | −0.003 (3) | −0.018 (3) | −0.016 (3) |
| C4 | 0.068 (3) | 0.064 (3) | 0.030 (2) | −0.005 (3) | −0.006 (2) | −0.002 (2) |
| C5 | 0.039 (2) | 0.039 (2) | 0.029 (2) | 0.0052 (18) | −0.0038 (18) | −0.0028 (17) |
| C6 | 0.036 (2) | 0.034 (2) | 0.036 (2) | 0.0076 (18) | −0.0032 (18) | 0.0004 (17) |
| C7 | 0.051 (3) | 0.048 (3) | 0.047 (3) | 0.000 (2) | 0.001 (2) | 0.006 (2) |
| C8 | 0.060 (3) | 0.048 (3) | 0.074 (4) | −0.015 (3) | 0.006 (3) | 0.008 (3) |
| C9 | 0.065 (4) | 0.049 (3) | 0.078 (4) | −0.016 (3) | −0.009 (3) | −0.008 (3) |
| C10 | 0.059 (3) | 0.045 (3) | 0.053 (3) | −0.008 (2) | −0.008 (2) | −0.009 (2) |
| C11 | 0.059 (3) | 0.043 (3) | 0.043 (3) | 0.006 (2) | −0.005 (2) | 0.000 (2) |
| C12 | 0.070 (4) | 0.055 (3) | 0.054 (3) | 0.027 (3) | −0.012 (3) | −0.009 (2) |
| C13 | 0.052 (3) | 0.073 (4) | 0.067 (3) | 0.028 (3) | −0.012 (3) | −0.027 (3) |
| C14 | 0.038 (3) | 0.067 (3) | 0.057 (3) | 0.009 (2) | 0.000 (2) | −0.021 (3) |
| C15 | 0.035 (2) | 0.049 (2) | 0.027 (2) | 0.0061 (19) | −0.0053 (17) | −0.0140 (18) |
| C16 | 0.032 (2) | 0.048 (2) | 0.0248 (19) | −0.0017 (18) | −0.0056 (16) | −0.0114 (17) |
| C17 | 0.037 (2) | 0.058 (3) | 0.035 (2) | −0.008 (2) | 0.0010 (19) | −0.010 (2) |
| C18 | 0.061 (3) | 0.056 (3) | 0.039 (2) | −0.023 (3) | −0.005 (2) | −0.003 (2) |
| C19 | 0.061 (3) | 0.039 (2) | 0.046 (3) | −0.007 (2) | −0.012 (2) | −0.002 (2) |
| C20 | 0.043 (3) | 0.040 (2) | 0.039 (2) | 0.0033 (19) | −0.0093 (19) | −0.0043 (19) |
| C21 | 0.035 (2) | 0.038 (2) | 0.0276 (19) | −0.0058 (18) | −0.0065 (17) | −0.0046 (17) |
| C22 | 0.042 (3) | 0.045 (2) | 0.043 (2) | 0.009 (2) | −0.017 (2) | −0.014 (2) |
| C23 | 0.053 (3) | 0.046 (3) | 0.037 (2) | 0.006 (2) | −0.013 (2) | −0.015 (2) |
| C24 | 0.044 (3) | 0.044 (2) | 0.044 (2) | 0.009 (2) | −0.012 (2) | −0.015 (2) |
Geometric parameters (Å, °) top
| Cu1—O1 | 1.981 (3) | C4—C5 | 1.389 (6) |
| Cu1—N2 | 2.000 (4) | C4—H4A | 0.9300 |
| Cu1—N4 | 2.013 (3) | C5—C6 | 1.476 (7) |
| Cu1—N1 | 2.033 (3) | C6—C7 | 1.371 (6) |
| Cu1—N3 | 2.172 (3) | C7—C8 | 1.381 (8) |
| Cu1—O2 | 2.795 (3) | C7—H7A | 0.9300 |
| N1—C5 | 1.347 (5) | C8—C9 | 1.371 (8) |
| N1—C1 | 1.349 (6) | C8—H8A | 0.9300 |
| N2—C10 | 1.343 (6) | C9—C10 | 1.370 (7) |
| N2—C6 | 1.346 (5) | C9—H9A | 0.9300 |
| N3—C11 | 1.340 (6) | C10—H10A | 0.9300 |
| N3—C15 | 1.345 (6) | C11—C12 | 1.376 (7) |
| N4—C20 | 1.349 (5) | C11—H11A | 0.9300 |
| N4—C16 | 1.349 (5) | C12—C13 | 1.363 (8) |
| O1—C21 | 1.271 (5) | C12—H12A | 0.9300 |
| O2—C21 | 1.246 (5) | C13—C14 | 1.385 (8) |
| O3—C23 | 1.240 (6) | C13—H13A | 0.9300 |
| O4—C23 | 1.254 (6) | C14—C15 | 1.377 (6) |
| O5—H5B | 0.8457 | C14—H14A | 0.9300 |
| O5—H5C | 0.8510 | C15—C16 | 1.491 (6) |
| O6—H6B | 0.8421 | C16—C17 | 1.385 (6) |
| O6—H6C | 0.8584 | C17—C18 | 1.381 (7) |
| O7—H7B | 0.8517 | C17—H17A | 0.9300 |
| O7—H7C | 0.8424 | C18—C19 | 1.368 (7) |
| O8—H8B | 0.8491 | C18—H18A | 0.9300 |
| O8—H8C | 0.8459 | C19—C20 | 1.375 (6) |
| O9—H9B | 0.8404 | C19—H19A | 0.9300 |
| O9—H9C | 0.8548 | C20—H20A | 0.9300 |
| O10—H10B | 0.8424 | C21—C22 | 1.516 (6) |
| O10—H10C | 0.8505 | C22—C22i | 1.499 (8) |
| C1—C2 | 1.381 (7) | C22—H22A | 0.9700 |
| C1—H1A | 0.9300 | C22—H22B | 0.9700 |
| C2—C3 | 1.360 (8) | C23—C24 | 1.536 (6) |
| C2—H2A | 0.9300 | C24—C24ii | 1.511 (8) |
| C3—C4 | 1.378 (8) | C24—H24A | 0.9700 |
| C3—H3A | 0.9300 | C24—H24B | 0.9700 |
| | | |
| O1—Cu1—N2 | 92.51 (14) | C9—C8—H8A | 120.5 |
| O1—Cu1—N4 | 90.27 (13) | C7—C8—H8A | 120.5 |
| N2—Cu1—N4 | 176.56 (14) | C10—C9—C8 | 119.4 (6) |
| O1—Cu1—N1 | 159.82 (13) | C10—C9—H9A | 120.3 |
| N2—Cu1—N1 | 80.65 (15) | C8—C9—H9A | 120.3 |
| N4—Cu1—N1 | 96.06 (14) | N2—C10—C9 | 121.9 (5) |
| O1—Cu1—N3 | 101.12 (12) | N2—C10—H10A | 119.1 |
| N2—Cu1—N3 | 102.72 (14) | C9—C10—H10A | 119.1 |
| N4—Cu1—N3 | 78.70 (13) | N3—C11—C12 | 122.6 (5) |
| N1—Cu1—N3 | 98.90 (14) | N3—C11—H11A | 118.7 |
| O1—Cu1—O2 | 51.85 (10) | C12—C11—H11A | 118.7 |
| N2—Cu1—O2 | 86.73 (13) | C13—C12—C11 | 118.5 (5) |
| N4—Cu1—O2 | 93.40 (12) | C13—C12—H12A | 120.7 |
| N1—Cu1—O2 | 108.49 (12) | C11—C12—H12A | 120.7 |
| N3—Cu1—O2 | 152.18 (11) | C12—C13—C14 | 119.6 (5) |
| C5—N1—C1 | 118.7 (4) | C12—C13—H13A | 120.2 |
| C5—N1—Cu1 | 113.8 (3) | C14—C13—H13A | 120.2 |
| C1—N1—Cu1 | 127.3 (3) | C15—C14—C13 | 119.0 (5) |
| C10—N2—C6 | 118.7 (4) | C15—C14—H14A | 120.5 |
| C10—N2—Cu1 | 125.7 (3) | C13—C14—H14A | 120.5 |
| C6—N2—Cu1 | 115.6 (3) | N3—C15—C14 | 121.4 (4) |
| C11—N3—C15 | 118.7 (4) | N3—C15—C16 | 115.4 (4) |
| C11—N3—Cu1 | 128.5 (3) | C14—C15—C16 | 123.2 (4) |
| C15—N3—Cu1 | 112.3 (3) | N4—C16—C17 | 121.3 (4) |
| C20—N4—C16 | 118.7 (4) | N4—C16—C15 | 115.5 (4) |
| C20—N4—Cu1 | 123.6 (3) | C17—C16—C15 | 123.2 (4) |
| C16—N4—Cu1 | 117.4 (3) | C18—C17—C16 | 119.0 (4) |
| C21—O1—Cu1 | 111.5 (2) | C18—C17—H17A | 120.5 |
| C21—O2—Cu1 | 73.5 (2) | C16—C17—H17A | 120.5 |
| H5B—O5—H5C | 120.3 | C19—C18—C17 | 119.8 (4) |
| H6B—O6—H6C | 97.8 | C19—C18—H18A | 120.1 |
| H7B—O7—H7C | 97.0 | C17—C18—H18A | 120.1 |
| H8B—O8—H8C | 105.8 | C18—C19—C20 | 118.8 (4) |
| H9B—O9—H9C | 100.3 | C18—C19—H19A | 120.6 |
| H10B—O10—H10C | 104.9 | C20—C19—H19A | 120.6 |
| N1—C1—C2 | 121.8 (5) | N4—C20—C19 | 122.3 (4) |
| N1—C1—H1A | 119.1 | N4—C20—H20A | 118.8 |
| C2—C1—H1A | 119.1 | C19—C20—H20A | 118.8 |
| C3—C2—C1 | 119.3 (5) | O2—C21—O1 | 123.1 (4) |
| C3—C2—H2A | 120.4 | O2—C21—C22 | 119.7 (4) |
| C1—C2—H2A | 120.4 | O1—C21—C22 | 117.2 (3) |
| C2—C3—C4 | 119.9 (5) | C22i—C22—C21 | 114.7 (4) |
| C2—C3—H3A | 120.1 | C22i—C22—H22A | 108.6 |
| C4—C3—H3A | 120.1 | C21—C22—H22A | 108.6 |
| C3—C4—C5 | 118.7 (5) | C22i—C22—H22B | 108.6 |
| C3—C4—H4A | 120.6 | C21—C22—H22B | 108.6 |
| C5—C4—H4A | 120.6 | H22A—C22—H22B | 107.6 |
| N1—C5—C4 | 121.6 (4) | O3—C23—O4 | 123.4 (5) |
| N1—C5—C6 | 115.5 (4) | O3—C23—C24 | 119.0 (4) |
| C4—C5—C6 | 122.9 (4) | O4—C23—C24 | 117.5 (5) |
| N2—C6—C7 | 121.9 (5) | C24ii—C24—C23 | 110.8 (4) |
| N2—C6—C5 | 114.1 (4) | C24ii—C24—H24A | 109.5 |
| C7—C6—C5 | 124.0 (4) | C23—C24—H24A | 109.5 |
| C6—C7—C8 | 119.1 (5) | C24ii—C24—H24B | 109.5 |
| C6—C7—H7A | 120.5 | C23—C24—H24B | 109.5 |
| C8—C7—H7A | 120.5 | H24A—C24—H24B | 108.1 |
| C9—C8—C7 | 119.0 (5) | | |
| | | |
| C23—C24—C24ii—C23ii | 180.000 (1) | | |
| Symmetry codes: (i) −x+1, −y+2, −z+1; (ii) −x+1, −y+1, −z+1. |
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O5—H5B···O10iii | 0.85 | 1.96 | 2.750 (6) | 154 |
| O5—H5C···O9 | 0.85 | 1.90 | 2.739 (6) | 169 |
| O6—H6B···O5 | 0.84 | 1.99 | 2.820 (6) | 168 |
| O6—H6C···O5iv | 0.86 | 2.01 | 2.847 (7) | 167 |
| O7—H7B···O6ii | 0.85 | 2.01 | 2.755 (5) | 146 |
| O7—H7C···O8 | 0.84 | 1.98 | 2.820 (5) | 175 |
| O8—H8B···O2v | 0.85 | 1.95 | 2.795 (5) | 177 |
| O8—H8C···O3 | 0.85 | 1.85 | 2.682 (5) | 169 |
| O9—H9B···O8ii | 0.84 | 2.02 | 2.850 (5) | 172 |
| O9—H9C···O4 | 0.86 | 1.85 | 2.704 (6) | 176 |
| O10—H10B···O7vi | 0.84 | 2.09 | 2.877 (7) | 156 |
| O10—H10C···O4 | 0.85 | 1.99 | 2.758 (7) | 149 |
| Symmetry codes: (iii) −x+1, −y+1, −z; (iv) −x+2, −y+1, −z; (ii) −x+1, −y+1, −z+1; (v) x, y−1, z; (vi) −x, −y+1, −z+1. |
Table 1
Hydrogen-bond geometry (Å, °) top
| D—H···A | D—H | H···A | D···A | D—H···A |
| O5—H5B···O10i | 0.85 | 1.96 | 2.750 (6) | 154 |
| O5—H5C···O9 | 0.85 | 1.90 | 2.739 (6) | 169 |
| O6—H6B···O5 | 0.84 | 1.99 | 2.820 (6) | 168 |
| O6—H6C···O5ii | 0.86 | 2.01 | 2.847 (7) | 167 |
| O7—H7B···O6iii | 0.85 | 2.01 | 2.755 (5) | 146 |
| O7—H7C···O8 | 0.84 | 1.98 | 2.820 (5) | 175 |
| O8—H8B···O2iv | 0.85 | 1.95 | 2.795 (5) | 177 |
| O8—H8C···O3 | 0.85 | 1.85 | 2.682 (5) | 169 |
| O9—H9B···O8iii | 0.84 | 2.02 | 2.850 (5) | 172 |
| O9—H9C···O4 | 0.86 | 1.85 | 2.704 (6) | 176 |
| O10—H10B···O7v | 0.84 | 2.09 | 2.877 (7) | 156 |
| O10—H10C···O4 | 0.85 | 1.99 | 2.758 (7) | 149 |
| Symmetry codes: (i) −x+1, −y+1, −z; (ii) −x+2, −y+1, −z; (iii) −x+1, −y+1, −z+1; (iv) x, y−1, z; (v) −x, −y+1, −z+1. |
This project was sponsored by the K. C. Wong Magna Fund in Ningbo University,
the Expert Project of Key Basic Research of the Ministry of Science and
Technology of China (grant No. 2003CCA00800), the Ningbo Municipal Natural
Science Foundation (grant No. 2006 A610061) and the Scientific Research Fund
of Ningbo University (grant No. XYL08012).
Batten, S. R. & Robson, R. (1998). Angew. Chem. Int. Ed. 37, 1460–1494.
Rao, C. N. R., Natarajan, S. & Vaidhyanathan, R. (2004). Angew. Chem. Int. Ed. 43, 1466–1496.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Siemens (1996). XSCANS. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
Wei, M. L., He, C., Hua, W. J., Duan, C. Y., Li, S. H. & Meng, Q. J. (2006). J. Am. Chem. Soc. 128, 13318–13319.
Zheng, Y. Q., Lin, J. L. & Kong, Z. P. (2004). Inorg. Chem. 43, 2590–2596.
In the past decade, metal-organic coordination polymers have attracted considerable interest due to their potential applications and intriguing architectures (Batten & Robson, 1998). The saturated aliphatic dicarboxylate ligands, which exhibit conformational and coordination versatility due to single-bonded carbon chains, are also an attractive choice and considered as important flexible spacer ligand (Rao, et al., 2004). As one of the lower members in the α,ω-dicarboxylate family, the succinate anions play a special role. Under ambient conditions, the linkage of transition metal cations by succinate anions may lead to linear polymeric chains, two-dimensional open networks and three-dimensional framework coordination polymers (Zheng, et al., 2004). Some metal-organic coordination polymers are open-frameworked and there are guest species occluded by open-framework host in the structures. Water molecules are the commonly encountered guest species, and they usually play an important role in the stabilization of the host, on the other hand, the configuration of water clusters depends on the surrounding environment of the host (Wei, et al., 2006). A variety of water clusters observed in a number of hosts have been structurally characterized to help us gain insight into the nature of water-water interactions. Herein, we report the presence of a new type (H2O)12 water cluster in the structure of succinato bridged dinuclear complex [Cu2(bpy)4(C4H4O4)](C4H4O4).12H2O.
The title compound consists of succinato bridged dinuclear [Cu2(bpy)4(C4H4O4)]2+ complex cations, succinate anions and crystal water molecules. As illustrated in Fig. 1, Cu2+ in the complex cations are each square pyramidally coordinated by one O atom of the succinato ligand and four N atoms of two bpy ligands with the N3 atom at the apical position (d(Cu—O) = 1.981 (3) Å; equatorial d(Cu—N) = 2.000 (4)–2.033 (3) Å; axial d(Cu—N) = 2.172 (3) Å). The Cu atom is shift by 0.179 (2) from the equatorial plane through N1, N2, N4 and O4 atoms towards the apical N3 atom. The succinato group bis-bidentately bridges two Cu ions to form the dinuclear complex cation. Such bridging succinato ligand and the noncoordinating succinate anion are also exhibit trans conformation with the backbone C atoms in a plane. The dehedral angles between the two pyridine rings are twisted by 8.34° and 10.08° in the two different bpy ligands. The complex cations are forced to be aligned in such ways that the symmetry related bpy ligands are orientated parallelly and face the opposite directions with the interplanar distanceds varying from 3.533 Å to 3.541 Å. Obviously, sucn π-π stacking interactions are responsible for the supramolecular assembly of the complex molecules into two-dimensional layers parallel to (010). The resulting complex cationic layers are found to be stabilized by weak C(bpy)-H···O(carboxylate) hydrogen bonds with d(H4A···O2II) = 2.47 Å (II: -x, -y + 2, -z + 2) (Fig. 2).
The most interesting feature of the solid-state structure of the title complex is the hydrogen-bonding interactions of the water molecules and the succinate anion, in which twelve water molecules form a (H2O)12 cluster associated by O—H···O hydrogen bonds (as shown in Fig 3). The geometric parameters of the clusters are summarized in Tables 1. The O···O distances range from 2.738 (6)–2.876 (7) Å and the angles of the O—H···O are vary from 145° to 175°. Interestingly, such (H2O)12 water clusters are farther hydrogen bond interacting with succinate anions to complete two-dimensional layers parallel to (010) with (d(O···O) = 2.682 (5)–2.758 (7) Å; <O—H···O = 149–176°).