supplementary materials


Acta Cryst. (2007). E63, m2414    [ doi:10.1107/S1600536807041190 ]

Hexaaquacopper(II) bis(4-hydroxybenzenesulfonate)

Y.-Q. Liu and X.-R. Zeng

Abstract top

The title complex, [Cu(H2O)6](C6H5SO4)2, was synthesized hydrothermally. The [Cu(H2O)6]2+ cations lie on centres of symmetry and exhibit tetragonally elongated coordination geometry, typical of Jahn-Teller-distorted CuII complexes. An extensive network of O-H...O hydrogen bonds between the coordinated water molecules and the sulfonate groups of the anions links the molecules into layers. The hydroxy groups of the anions form O-H...O hydrogen bonds that link between layers.

Comment top

In the title complex (Fig. 1), the [Cu(H2O)6]2+ cations lies on centres of symmetry and exhibit tetragonally elongated coordination geometry, with atoms O2, O3, O2i and O3i forming the equatorial plane and atoms O1 and O1i lying in the axial positions [symmetry code (i): 1 − x, 2 − y, −z]. The Cu1—O1 bond length of 2.3842 (14) Å is significantly longer than the Cu1—O2 and Cu1—O3 bond lengths of 1.9645 (14) and 1.9615 (13) Å, respectively.

An extensive network of O—H···O hydrogen bonds between the coordinated water molecules and the sulfonate groups of the anions link the molecules into layers lying in the (002) planes (Fig. 2). The hydroxy groups of the anions form O—H···O hydrogen bonds between layers.

Related literature top

For the structure of a related complex [Ni(H2O)6](C6H5SO4)2·2H2O, see: Kosnic et al. (1992).

Experimental top

A mixture of 4-hydroxybenzenesulfonic acid (0.348 g, 0.002 mol) and CuO (0.079, 0.001 mol) was added to 20 ml water and the mixture was sealed in a teflon-lined steel autoclave and heated at 418 K for 4 days. Single crystals of the title compound formed on cooling in air.

Refinement top

H atoms bound to C atoms and of the OH group were placed geometrically and refined as riding with C—H = 0.93 Å and O—H = 0.82 Å, and with Ueq(H) = 1.2 Ueq(C) or 1.5 Ueq(O). The H atoms of the water molecules were located in difference Fourier maps and refined with the O—H bond lengths restrained to 0.83 (2) Å and with Uiso(H) refined freely.

Computing details top

Data collection: APEX2 (Bruker, 2000); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1997); software used to prepare material for publication: SHELXTL (Bruker, 1997).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound showing 30% probability displacement ellipsoids. H atoms are omitted. The suffix A denotes symmetry code 1 − x, 2 − y, −z.
[Figure 2] Fig. 2. Packing diagram viewed along the a axis showing a layer in the (002) plane. Hydrogen bonds are shown as dashed lines.
Hexaaquacopper(II) bis(4-hydroxybenzenesulfonate) top
Crystal data top
[Cu(H2O)6](C6H5SO4)2F000 = 534.0
Mr = 517.99Dx = 1.706 Mg m3
Monoclinic, P21/nMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 6039 reflections
a = 6.9299 (13) Åθ = 2.6–28.3º
b = 6.1868 (12) ŵ = 1.36 mm1
c = 23.531 (4) ÅT = 293 (2) K
β = 91.528 (2)ºBlock, blue
V = 1008.5 (3) Å30.48 × 0.48 × 0.35 mm
Z = 2
Data collection top
Bruker SMART APEX II CCD
diffractometer
1833 independent reflections
Radiation source: fine-focus sealed tube1734 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.052
T = 293(2) Kθmax = 25.5º
φ and ω scansθmin = 3.1º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 8→8
Tmin = 0.530, Tmax = 0.620k = 7→7
5886 measured reflectionsl = 27→28
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.027H atoms treated by a mixture of
independent and constrained refinement
wR(F2) = 0.079  w = 1/[σ2(Fo2) + (0.05P)2 + 0.2229P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.002
1833 reflectionsΔρmax = 0.35 e Å3
159 parametersΔρmin = 0.29 e Å3
9 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.073 (4)
Crystal data top
[Cu(H2O)6](C6H5SO4)2V = 1008.5 (3) Å3
Mr = 517.99Z = 2
Monoclinic, P21/nMo Kα
a = 6.9299 (13) ŵ = 1.36 mm1
b = 6.1868 (12) ÅT = 293 (2) K
c = 23.531 (4) Å0.48 × 0.48 × 0.35 mm
β = 91.528 (2)º
Data collection top
Bruker SMART APEX II CCD
diffractometer
1833 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1734 reflections with I > 2σ(I)
Tmin = 0.530, Tmax = 0.620Rint = 0.052
5886 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0279 restraints
wR(F2) = 0.079H atoms treated by a mixture of
independent and constrained refinement
S = 1.09Δρmax = 0.35 e Å3
1833 reflectionsΔρmin = 0.29 e Å3
159 parameters
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 > 2sigma(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
xyzUiso*/Ueq
Cu10.50001.00000.00000.03006 (16)
S10.00308 (6)0.60798 (7)0.098056 (18)0.03163 (17)
C30.0610 (3)0.6358 (4)0.26714 (9)0.0446 (5)
H30.10900.73340.29330.053*
C60.0787 (3)0.3434 (3)0.18887 (8)0.0391 (4)
H60.12540.24550.16260.047*
C20.0607 (3)0.6884 (3)0.21002 (9)0.0415 (5)
H20.10750.82190.19780.050*
C10.0092 (3)0.5428 (3)0.17107 (8)0.0330 (4)
C50.0783 (3)0.2909 (4)0.24607 (9)0.0430 (5)
H50.12380.15660.25820.052*
C40.0103 (3)0.4375 (4)0.28548 (9)0.0427 (5)
O30.4870 (2)0.7127 (2)0.03289 (6)0.0377 (3)
O60.1696 (2)0.5037 (2)0.07292 (7)0.0407 (4)
O10.6894 (2)1.1065 (2)0.08131 (6)0.0424 (4)
O20.2623 (2)1.0915 (2)0.03679 (7)0.0476 (4)
O50.1792 (2)0.5252 (2)0.07440 (7)0.0431 (4)
O40.0127 (2)0.8432 (2)0.09386 (6)0.0416 (4)
O70.0198 (3)0.3770 (3)0.34066 (6)0.0596 (5)
H70.02490.47310.36040.089*
H1A0.7892 (16)1.032 (3)0.0829 (13)0.053 (8)*
H2A0.234 (3)1.2081 (16)0.0517 (9)0.062 (8)*
H3A0.395 (2)0.662 (4)0.0504 (9)0.052 (7)*
H1B0.741 (3)1.2271 (14)0.0803 (14)0.069 (9)*
H2B0.193 (3)1.012 (2)0.0558 (10)0.052 (8)*
H3B0.575 (2)0.653 (4)0.0513 (10)0.079 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0321 (2)0.0257 (2)0.0325 (2)0.00063 (11)0.00330 (13)0.00130 (11)
S10.0316 (3)0.0290 (3)0.0342 (3)0.00129 (17)0.00018 (17)0.00307 (17)
C30.0422 (11)0.0510 (12)0.0407 (11)0.0057 (9)0.0051 (8)0.0053 (9)
C60.0415 (11)0.0383 (10)0.0374 (10)0.0047 (8)0.0003 (7)0.0003 (8)
C20.0396 (11)0.0403 (11)0.0447 (11)0.0068 (8)0.0012 (8)0.0002 (9)
C10.0291 (9)0.0353 (9)0.0344 (9)0.0009 (7)0.0011 (7)0.0019 (8)
C50.0438 (11)0.0420 (11)0.0431 (11)0.0061 (9)0.0025 (8)0.0074 (9)
C40.0365 (11)0.0554 (12)0.0359 (10)0.0004 (10)0.0005 (7)0.0036 (9)
O30.0354 (7)0.0305 (7)0.0474 (8)0.0011 (6)0.0016 (6)0.0074 (6)
O60.0424 (9)0.0372 (8)0.0430 (8)0.0019 (5)0.0085 (6)0.0007 (5)
O10.0402 (8)0.0347 (8)0.0519 (8)0.0026 (6)0.0046 (6)0.0013 (6)
O20.0479 (9)0.0306 (8)0.0654 (10)0.0017 (7)0.0241 (7)0.0018 (7)
O50.0400 (8)0.0415 (8)0.0469 (9)0.0062 (6)0.0113 (6)0.0066 (6)
O40.0435 (8)0.0305 (7)0.0511 (8)0.0011 (5)0.0032 (6)0.0058 (6)
O70.0698 (11)0.0737 (12)0.0353 (8)0.0148 (9)0.0028 (7)0.0072 (8)
Geometric parameters (Å, °) top
Cu1—O12.3842 (14)C6—C11.385 (3)
Cu1—O21.9645 (14)C6—H60.930
Cu1—O31.9415 (13)C2—C11.382 (3)
Cu1—O1i2.3842 (14)C2—H20.930
Cu1—O2i1.9645 (14)C5—C41.389 (3)
Cu1—O3i1.9415 (13)C5—H50.930
S1—O41.4605 (15)C4—O71.351 (3)
S1—O51.4595 (15)O3—H3A0.83 (2)
S1—O61.4608 (16)O3—H3B0.83 (2)
S1—C11.7641 (19)O1—H1A0.83 (1)
C3—C21.383 (3)O1—H1B0.83 (1)
C3—C41.387 (3)O2—H2A0.83 (1)
C3—H30.930O2—H2B0.83 (2)
C6—C51.385 (3)O7—H70.820
O3i—Cu1—O3180.00 (8)C5—C6—H6120.2
O3i—Cu1—O2i92.28 (6)C1—C6—H6120.2
O3—Cu1—O2i87.72 (6)C1—C2—C3120.05 (19)
O3i—Cu1—O287.72 (6)C1—C2—H2120.0
O3—Cu1—O292.28 (6)C3—C2—H2120.0
O2i—Cu1—O2180.00 (12)C2—C1—C6120.34 (18)
O3i—Cu1—O192.10 (6)C2—C1—S1119.81 (15)
O3—Cu1—O187.90 (6)C6—C1—S1119.82 (15)
O2i—Cu1—O189.03 (6)C4—C5—C6120.3 (2)
O2—Cu1—O190.97 (6)C4—C5—H5119.8
O3i—Cu1—O1i87.90 (6)C6—C5—H5119.8
O3—Cu1—O1i92.10 (6)O7—C4—C5116.9 (2)
O2i—Cu1—O1i90.97 (6)O7—C4—C3123.5 (2)
O2—Cu1—O1i89.03 (6)C5—C4—C3119.64 (19)
O1—Cu1—O1i180.0Cu1—O3—H3A126.0 (16)
O4—S1—O5111.39 (8)Cu1—O3—H3B125.3 (17)
O4—S1—O6112.00 (8)H3A—O3—H3B97.9 (19)
O5—S1—O6112.05 (9)Cu1—O1—H1A108.8 (19)
O4—S1—C1107.08 (9)Cu1—O1—H1B117 (2)
O5—S1—C1106.82 (9)H1A—O1—H1B98.1 (18)
O6—S1—C1107.14 (9)Cu1—O2—H2A130.5 (15)
C2—C3—C4120.05 (19)Cu1—O2—H2B125.1 (15)
C2—C3—H3120.0H2A—O2—H2B98.1 (18)
C4—C3—H3120.0C4—O7—H7109.5
C5—C6—C1119.58 (19)
Symmetry codes: (i) −x+1, −y+2, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O7—H7···O1ii0.821.992.763 (2)158
O1—H1A···O4iii0.83 (1)1.95 (2)2.779 (2)174 (3)
O1—H1B···O5iv0.83 (1)1.93 (1)2.752 (2)171 (2)
O2—H2B···O40.83 (2)1.87 (2)2.698 (2)174 (3)
O2—H2A···O6v0.83 (1)1.95 (1)2.769 (2)170 (2)
O3—H3B···O5iii0.83 (2)1.94 (2)2.744 (2)164 (2)
O3—H3A···O60.83 (2)1.93 (2)2.740 (2)165 (3)
Symmetry codes: (ii) −x+1/2, y−1/2, −z+1/2; (iii) x+1, y, z; (iv) x+1, y+1, z; (v) x, y+1, z.
Selected geometric parameters (Å) top
Cu1—O12.3842 (14)Cu1—O31.9415 (13)
Cu1—O21.9645 (14)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O7—H7···O1i0.821.992.763 (2)158
O1—H1A···O4ii0.83 (1)1.95 (2)2.779 (2)174 (3)
O1—H1B···O5iii0.83 (1)1.93 (1)2.752 (2)171 (2)
O2—H2B···O40.83 (2)1.87 (2)2.698 (2)174 (3)
O2—H2A···O6iv0.83 (1)1.95 (1)2.769 (2)170 (2)
O3—H3B···O5ii0.83 (2)1.94 (2)2.744 (2)164 (2)
O3—H3A···O60.83 (2)1.93 (2)2.740 (2)165 (3)
Symmetry codes: (i) −x+1/2, y−1/2, −z+1/2; (ii) x+1, y, z; (iii) x+1, y+1, z; (iv) x, y+1, z.
Acknowledgements top

The authors are grateful for the support of this work by the Natural Science Foundation of JiangXi Province (grant Nos. 0520036 and 0620029).

references
References top

Bruker (1997). SAINT and SHELXTL. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2000). (DATE?). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA.

Kosnic, E. J., McClymont, E. L., Hodder, R. A. & Squattrito, P. J. (1992). Inorg. Chim. Acta, 201, 143–151.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.