Buy article online - an online subscription or single-article purchase is required to access this article.
In the title compound, {[Cu2(SO4)2(C3H6N2O2)2(H2O)4]·2H2O}, two differently coordinated Cu atoms are bridged by the sulfate groups, forming a polymeric chain extending along the c axis. One Cu atom is coordinated by two malonamide molecules and two sulfate groups, while the other is coordinated by four water molecules and two sulfate groups. Both Cu atoms lie on centers of symmetry. An extensive three-dimensional hydrogen-bonding network involves the uncoordinated water molecules and stabilizes the crystal packing.
Supporting information
CCDC reference: 610740
Key indicators
- Single-crystal X-ray study
- T = 120 K
- Mean (C-C) = 0.005 Å
- R factor = 0.039
- wR factor = 0.097
- Data-to-parameter ratio = 13.5
checkCIF/PLATON results
No syntax errors found
Alert level C
PLAT041_ALERT_1_C Calc. and Rep. SumFormula Strings Differ .... ?
PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ?
PLAT045_ALERT_1_C Calculated and Reported Z Differ by ............ 2.00 Ratio
PLAT720_ALERT_4_C Number of Unusual/Non-Standard Label(s) ........ 6
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
4 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
3 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
Data collection: SMART (Bruker, 1998); cell refinement: SAINT-Plus (Bruker, 1998); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXTL (Sheldrick, 1998); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
catena-Poly[[[tetraaquacopper(II)]-µ-sulfato-
κ2O:
O'-
[bis(malonamide-
κ2O,
O')copper(II)]-µ-sulfato-
κ2O:
O'] dihydrate]
top
Crystal data top
[Cu2(SO4)2(C3H6N2O2)2(H2O)4]·2H2O | Z = 1 |
Mr = 631.50 | F(000) = 322 |
Triclinic, P1 | Dx = 2.028 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.7953 (10) Å | Cell parameters from 3044 reflections |
b = 7.1236 (11) Å | θ = 6.4–52.0° |
c = 12.2249 (19) Å | µ = 2.35 mm−1 |
α = 78.692 (3)° | T = 120 K |
β = 77.817 (3)° | Prism, blue |
γ = 64.214 (2)° | 0.15 × 0.15 × 0.1 mm |
V = 517.18 (14) Å3 | |
Data collection top
Bruker SMART 1000 CCD area-detector diffractometer | 1996 independent reflections |
Radiation source: normal-focus sealed tube | 1813 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.032 |
φ and ω scans | θmax = 26.0°, θmin = 3.4° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | h = −8→8 |
Tmin = 0.684, Tmax = 0.790 | k = −8→8 |
4014 measured reflections | l = −14→15 |
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)] = 0.039 | Hydrogen site location: mixed |
wR(F2) = 0.098 | H-atom parameters constrained |
S = 1.00 | w = 1/[σ2(Fo2) + (0.045P)2 + 2.25P] where P = (Fo2 + 2Fc2)/3 |
1996 reflections | (Δ/σ)max < 0.001 |
148 parameters | Δρmax = 0.92 e Å−3 |
0 restraints | Δρmin = −1.12 e Å−3 |
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 | 0.5000 | 0.0000 | 0.0000 | 0.00867 (17) | |
Cu2 | 0.5000 | 0.0000 | −0.5000 | 0.00968 (17) | |
S1 | 0.80296 (13) | −0.10775 (12) | −0.27311 (7) | 0.0089 (2) | |
O1 | 0.7350 (4) | −0.0142 (4) | −0.1673 (2) | 0.0144 (5) | |
O2 | 0.6801 (4) | 0.0449 (4) | −0.3628 (2) | 0.0127 (5) | |
O3 | 0.7612 (4) | −0.2990 (4) | −0.2587 (2) | 0.0130 (5) | |
O4 | 1.0448 (4) | −0.1663 (4) | −0.3082 (2) | 0.0129 (5) | |
O5 | 0.5661 (4) | −0.3007 (4) | 0.0253 (2) | 0.0117 (5) | |
O6 | 0.7546 (4) | −0.0391 (4) | 0.0686 (2) | 0.0117 (5) | |
O7 | 0.5465 (4) | −0.2790 (4) | −0.4181 (2) | 0.0119 (5) | |
H7A | 0.6161 | −0.2935 | −0.3675 | 0.018* | |
H7B | 0.6227 | −0.3730 | −0.4578 | 0.018* | |
O8 | 0.2143 (4) | 0.1182 (4) | −0.4022 (2) | 0.0130 (5) | |
H8A | 0.1096 | 0.2041 | −0.4336 | 0.020* | |
H8B | 0.1848 | 0.0247 | −0.3619 | 0.020* | |
N1 | 0.6786 (5) | −0.6172 (5) | 0.1273 (3) | 0.0159 (6) | |
H1N1 | 0.7598 | −0.7023 | 0.1810 | 0.019* | |
H2N1 | 0.6111 | −0.6556 | 0.0854 | 0.019* | |
N2 | 1.0589 (5) | −0.2615 (5) | 0.1450 (3) | 0.0151 (6) | |
H1N2 | 1.1322 | −0.3846 | 0.1850 | 0.018* | |
H2N2 | 1.1238 | −0.1722 | 0.1173 | 0.018* | |
C1 | 0.6601 (5) | −0.4235 (5) | 0.1063 (3) | 0.0095 (6) | |
C2 | 0.7479 (5) | −0.3524 (5) | 0.1857 (3) | 0.0103 (7) | |
H2A | 0.8565 | −0.4773 | 0.2252 | 0.012* | |
H2B | 0.6247 | −0.2797 | 0.2432 | 0.012* | |
C3 | 0.8565 (5) | −0.2073 (5) | 0.1280 (3) | 0.0110 (7) | |
O1W | 1.1794 (4) | −0.3421 (4) | −0.5112 (2) | 0.0139 (5) | |
H1W1 | 1.1862 | −0.3205 | −0.4489 | 0.021* | |
H2W1 | 1.2466 | −0.2851 | −0.5592 | 0.021* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cu1 | 0.0093 (3) | 0.0077 (3) | 0.0106 (3) | −0.0042 (2) | −0.0042 (2) | 0.0000 (2) |
Cu2 | 0.0083 (3) | 0.0093 (3) | 0.0112 (3) | −0.0033 (2) | −0.0015 (2) | −0.0010 (2) |
S1 | 0.0085 (4) | 0.0103 (4) | 0.0090 (4) | −0.0043 (3) | −0.0025 (3) | −0.0010 (3) |
O1 | 0.0151 (12) | 0.0205 (13) | 0.0105 (12) | −0.0093 (10) | −0.0009 (9) | −0.0043 (10) |
O2 | 0.0138 (12) | 0.0106 (11) | 0.0124 (12) | −0.0039 (9) | −0.0048 (9) | 0.0021 (9) |
O3 | 0.0165 (12) | 0.0103 (11) | 0.0161 (12) | −0.0081 (10) | −0.0063 (10) | 0.0008 (9) |
O4 | 0.0096 (12) | 0.0144 (12) | 0.0131 (12) | −0.0041 (10) | −0.0011 (9) | −0.0007 (9) |
O5 | 0.0128 (12) | 0.0117 (12) | 0.0124 (12) | −0.0054 (9) | −0.0052 (9) | −0.0009 (9) |
O6 | 0.0133 (12) | 0.0103 (11) | 0.0141 (12) | −0.0062 (9) | −0.0054 (9) | −0.0002 (9) |
O7 | 0.0133 (12) | 0.0104 (11) | 0.0126 (12) | −0.0042 (9) | −0.0047 (9) | −0.0008 (9) |
O8 | 0.0114 (12) | 0.0131 (12) | 0.0142 (12) | −0.0048 (9) | −0.0026 (10) | −0.0004 (9) |
N1 | 0.0226 (16) | 0.0121 (14) | 0.0188 (15) | −0.0096 (12) | −0.0132 (13) | 0.0028 (12) |
N2 | 0.0117 (14) | 0.0131 (14) | 0.0216 (16) | −0.0059 (12) | −0.0076 (12) | 0.0028 (12) |
C1 | 0.0069 (15) | 0.0108 (15) | 0.0105 (15) | −0.0027 (12) | −0.0019 (12) | −0.0023 (12) |
C2 | 0.0108 (15) | 0.0097 (15) | 0.0117 (15) | −0.0046 (13) | −0.0035 (13) | −0.0010 (12) |
C3 | 0.0123 (16) | 0.0103 (15) | 0.0118 (16) | −0.0044 (13) | −0.0024 (13) | −0.0041 (12) |
O1W | 0.0164 (12) | 0.0146 (12) | 0.0129 (12) | −0.0084 (10) | −0.0015 (10) | −0.0020 (9) |
Geometric parameters (Å, º) top
Cu1—O1 | 2.304 (2) | O6—C3 | 1.262 (4) |
Cu1—O1i | 2.304 (2) | O7—H7A | 0.8201 |
Cu1—O5i | 1.962 (2) | O7—H7B | 0.8200 |
Cu1—O5 | 1.962 (2) | O8—H8A | 0.8201 |
Cu1—O6i | 1.969 (2) | O8—H8B | 0.8200 |
Cu1—O6 | 1.969 (2) | N1—C1 | 1.308 (4) |
Cu2—O2ii | 2.415 (2) | N1—H1N1 | 0.9000 |
Cu2—O2 | 2.415 (2) | N1—H2N1 | 0.9001 |
Cu2—O7ii | 1.964 (2) | N2—C3 | 1.308 (5) |
Cu2—O7 | 1.964 (2) | N2—H1N2 | 0.9000 |
Cu2—O8 | 1.975 (2) | N2—H2N2 | 0.9000 |
Cu2—O8ii | 1.975 (2) | C1—C2 | 1.501 (5) |
S1—O1 | 1.465 (3) | C2—C3 | 1.506 (4) |
S1—O3 | 1.480 (2) | C2—H2A | 0.9900 |
S1—O2 | 1.486 (2) | C2—H2B | 0.9900 |
S1—O4 | 1.495 (2) | O1W—H1W1 | 0.8199 |
O5—C1 | 1.262 (4) | O1W—H2W1 | 0.8200 |
| | | |
O5i—Cu1—O5 | 180.0 | O1—S1—O4 | 108.70 (14) |
O5i—Cu1—O1 | 84.37 (9) | O3—S1—O4 | 108.72 (14) |
O1—Cu1—O5 | 95.63 (9) | O2—S1—O4 | 109.25 (14) |
O6i—Cu1—O1 | 95.51 (9) | S1—O1—Cu1 | 141.05 (15) |
O1—Cu1—O6 | 84.49 (9) | S1—O2—Cu2 | 130.66 (14) |
O5i—Cu1—O6i | 93.11 (10) | C1—O5—Cu1 | 123.5 (2) |
O5—Cu1—O6i | 86.89 (10) | C3—O6—Cu1 | 121.7 (2) |
O5i—Cu1—O6 | 86.89 (10) | Cu2—O7—H7A | 105.5 |
O5—Cu1—O6 | 93.11 (10) | Cu2—O7—H7B | 112.0 |
O6i—Cu1—O6 | 180.00 (17) | H7A—O7—H7B | 107.2 |
O5i—Cu1—O1i | 95.63 (9) | Cu2—O8—H8A | 116.3 |
O5—Cu1—O1i | 84.37 (9) | Cu2—O8—H8B | 110.9 |
O6i—Cu1—O1i | 84.49 (9) | H8A—O8—H8B | 111.8 |
O6—Cu1—O1i | 95.51 (9) | C1—N1—H1N1 | 117.8 |
O1—Cu1—O1i | 180.00 (18) | C1—N1—H2N1 | 117.1 |
O7ii—Cu2—O7 | 180.00 (13) | H1N1—N1—H2N1 | 125.1 |
O7ii—Cu2—O2 | 92.37 (9) | C3—N2—H1N2 | 121.0 |
O2—Cu2—O7 | 87.63 (9) | C3—N2—H2N2 | 119.0 |
O8—Cu2—O2ii | 90.61 (9) | H1N2—N2—H2N2 | 120.0 |
O8ii—Cu2—O2ii | 89.39 (9) | O5—C1—N1 | 121.3 (3) |
O2—Cu2—O8 | 89.39 (9) | O5—C1—C2 | 121.9 (3) |
O8ii—Cu2—O2 | 90.61 (9) | N1—C1—C2 | 116.8 (3) |
O7ii—Cu2—O8 | 91.09 (10) | C1—C2—C3 | 113.4 (3) |
O7—Cu2—O8 | 88.91 (10) | C1—C2—H2A | 108.9 |
O7ii—Cu2—O8ii | 88.91 (10) | C3—C2—H2A | 108.9 |
O7—Cu2—O8ii | 91.09 (10) | C1—C2—H2B | 108.9 |
O8—Cu2—O8ii | 180.0 | C3—C2—H2B | 108.9 |
O7ii—Cu2—O2ii | 87.63 (9) | H2A—C2—H2B | 107.7 |
O7—Cu2—O2ii | 92.37 (9) | O6—C3—N2 | 121.8 (3) |
O2ii—Cu2—O2 | 180.0 | O6—C3—C2 | 121.4 (3) |
O1—S1—O3 | 110.95 (14) | N2—C3—C2 | 116.8 (3) |
O1—S1—O2 | 110.31 (14) | H1W1—O1W—H2W1 | 108.5 |
O3—S1—O2 | 108.88 (14) | | |
| | | |
O3—S1—O1—Cu1 | −23.8 (3) | O6—Cu1—O5—C1 | 29.9 (3) |
O2—S1—O1—Cu1 | 96.9 (3) | O1—Cu1—O5—C1 | 114.6 (2) |
O4—S1—O1—Cu1 | −143.3 (2) | O1i—Cu1—O5—C1 | −65.4 (2) |
O5i—Cu1—O1—S1 | −136.4 (3) | O5i—Cu1—O6—C3 | 165.0 (3) |
O5—Cu1—O1—S1 | 43.6 (3) | O5—Cu1—O6—C3 | −15.0 (3) |
O6i—Cu1—O1—S1 | −43.8 (3) | O1—Cu1—O6—C3 | −110.4 (3) |
O6—Cu1—O1—S1 | 136.2 (3) | O1i—Cu1—O6—C3 | 69.6 (3) |
O1—S1—O2—Cu2 | −134.93 (17) | Cu1—O5—C1—N1 | 172.2 (2) |
O3—S1—O2—Cu2 | −13.0 (2) | Cu1—O5—C1—C2 | −5.3 (4) |
O4—S1—O2—Cu2 | 105.65 (18) | O5—C1—C2—C3 | −39.6 (4) |
O7ii—Cu2—O2—S1 | −170.30 (18) | N1—C1—C2—C3 | 142.8 (3) |
O7—Cu2—O2—S1 | 9.70 (18) | Cu1—O6—C3—N2 | 158.7 (3) |
O8—Cu2—O2—S1 | 98.64 (18) | Cu1—O6—C3—C2 | −23.1 (4) |
O8ii—Cu2—O2—S1 | −81.36 (18) | C1—C2—C3—O6 | 56.3 (4) |
O6i—Cu1—O5—C1 | −150.1 (3) | C1—C2—C3—N2 | −125.4 (3) |
Symmetry codes: (i) −x+1, −y, −z; (ii) −x+1, −y, −z−1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
O7—H7A···O3 | 0.82 | 1.80 | 2.618 (3) | 175 |
O7—H7B···O1Wiii | 0.82 | 1.95 | 2.714 (3) | 156 |
O8—H8A···O1Wii | 0.82 | 1.97 | 2.765 (3) | 162 |
O8—H8B···O4iv | 0.82 | 1.92 | 2.704 (3) | 159 |
N1—H1N1···O4v | 0.90 | 2.07 | 2.949 (4) | 166 |
N1—H2N1···O5vi | 0.90 | 2.14 | 3.029 (4) | 171 |
N2—H1N2···O3v | 0.90 | 2.12 | 2.985 (4) | 162 |
N2—H2N2···O1vii | 0.90 | 2.18 | 2.943 (4) | 143 |
O1W—H1W1···O4 | 0.82 | 2.05 | 2.798 (3) | 151 |
O1W—H2W1···O2viii | 0.82 | 2.00 | 2.761 (3) | 155 |
Symmetry codes: (ii) −x+1, −y, −z−1; (iii) −x+2, −y−1, −z−1; (iv) x−1, y, z; (v) −x+2, −y−1, −z; (vi) −x+1, −y−1, −z; (vii) −x+2, −y, −z; (viii) −x+2, −y, −z−1. |
Subscribe to Acta Crystallographica Section E: Crystallographic Communications
The full text of this article is available to subscribers to the journal.
If you have already registered and are using a computer listed in your registration details, please email
support@iucr.org for assistance.