Buy article online - an online subscription or single-article purchase is required to access this article.
Download citation
Download citation
link to html
In the title compound, [Cu(C2H8N2)2](C14H6O8S2), the CuII atom lies on an inversion centre and is coordinated by two ethyl­enediamine ligands in a square-planar geometry. 9,10-Dioxoanthracene-2,6-disulfonate anions, also lying on inversion centres, coordinate weakly to CuII and accept N—H...O hydrogen bonds from ethyl­enediamine, linking the [Cu(C2H8N2)2]2+ cations into chains. Adjacent chains are linked into extended two-dimensional networks via N—H...O hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807008215/bi2162sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807008215/bi2162Isup2.hkl
Contains datablock I

CCDC reference: 640264

Key indicators

  • Single-crystal X-ray study
  • T = 273 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.033
  • wR factor = 0.087
  • Data-to-parameter ratio = 14.8

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT042_ALERT_1_C Calc. and Rep. MoietyFormula Strings Differ .... ? PLAT094_ALERT_2_C Ratio of Maximum / Minimum Residual Density .... 2.13 PLAT154_ALERT_1_C The su's on the Cell Angles are Equal (x 10000) 300 Deg. PLAT333_ALERT_2_C Large Average Benzene C-C Dist. C4 -C7_b 1.45 Ang.
Alert level G PLAT804_ALERT_5_G ARU-Pack Problem in PLATON Analysis ............ 1 Times
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 2 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 0 ALERT type 4 Improvement, methodology, query or suggestion 1 ALERT type 5 Informative message, check

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; 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.

Bis(ethylenediamine-κ2N,N')copper(II) 9,10-dioxoanthracene-2,6-disulfonate top
Crystal data top
[Cu(C2H8N2)2](C14H6O8S2)Z = 1
Mr = 550.06F(000) = 283
Triclinic, P1Dx = 1.773 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 5.9738 (11) ÅCell parameters from 4412 reflections
b = 8.3196 (14) Åθ = 12–18°
c = 11.0372 (19) ŵ = 1.32 mm1
α = 79.231 (3)°T = 273 K
β = 78.946 (3)°Block, blue
γ = 75.258 (3)°0.32 × 0.26 × 0.20 mm
V = 515.11 (16) Å3
Data collection top
Bruker SMART CCD area-detector
diffractometer
2228 independent reflections
Radiation source: fine-focus sealed tube1760 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.019
ω scansθmax = 27.0°, θmin = 1.9°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 77
Tmin = 0.67, Tmax = 0.77k = 1010
4412 measured reflectionsl = 1414
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.087H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0406P)2 + 0.2691P]
where P = (Fo2 + 2Fc2)/3
2228 reflections(Δ/σ)max < 0.001
151 parametersΔρmax = 0.49 e Å3
0 restraintsΔρmin = 0.23 e Å3
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
xyzUiso*/Ueq
Cu10.00000.00000.50000.03089 (15)
S10.30573 (11)0.19633 (8)0.25059 (6)0.02894 (16)
O10.1407 (3)0.3498 (2)0.2788 (2)0.0463 (5)
O20.4030 (3)0.0987 (3)0.36019 (17)0.0415 (5)
O30.2160 (4)0.0968 (3)0.18533 (19)0.0469 (5)
O40.7449 (3)0.6970 (2)0.16757 (18)0.0412 (5)
N10.0702 (4)0.1022 (3)0.6340 (2)0.0340 (5)
H1A0.00840.05590.70930.041*
H1B0.22610.08340.63140.041*
N20.2309 (4)0.2193 (3)0.4660 (2)0.0339 (5)
H2A0.17500.28110.39610.041*
H2B0.36730.20080.45530.041*
C10.5428 (4)0.2597 (3)0.1453 (2)0.0253 (5)
C20.6675 (4)0.1612 (3)0.0547 (2)0.0308 (5)
H20.62420.06410.04740.037*
C30.8557 (4)0.2087 (3)0.0241 (2)0.0297 (5)
H30.93790.14390.08550.036*
C40.9239 (4)0.3528 (3)0.0127 (2)0.0247 (5)
C50.7957 (4)0.4525 (3)0.0770 (2)0.0238 (5)
C60.6032 (4)0.4060 (3)0.1557 (2)0.0262 (5)
H60.51600.47280.21490.031*
C70.8628 (4)0.6067 (3)0.0930 (2)0.0261 (5)
C80.0320 (6)0.2842 (4)0.6140 (3)0.0457 (7)
H8A0.06940.34040.55000.055*
H8B0.04990.33070.69050.055*
C90.2673 (5)0.3092 (4)0.5739 (3)0.0448 (7)
H9A0.37470.26470.64160.054*
H9B0.33280.42790.55080.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0393 (3)0.0274 (2)0.0276 (3)0.00766 (19)0.00812 (19)0.00460 (18)
S10.0268 (3)0.0330 (3)0.0284 (3)0.0147 (3)0.0017 (2)0.0006 (3)
O10.0340 (11)0.0399 (11)0.0571 (13)0.0091 (9)0.0099 (9)0.0037 (10)
O20.0419 (11)0.0503 (12)0.0315 (10)0.0176 (9)0.0063 (8)0.0068 (9)
O30.0473 (12)0.0614 (13)0.0432 (12)0.0356 (11)0.0035 (9)0.0064 (10)
O40.0389 (11)0.0414 (11)0.0460 (12)0.0165 (9)0.0110 (9)0.0211 (9)
N10.0412 (13)0.0335 (12)0.0304 (12)0.0144 (10)0.0071 (10)0.0025 (9)
N20.0335 (12)0.0355 (12)0.0334 (12)0.0102 (9)0.0037 (9)0.0053 (9)
C10.0227 (12)0.0304 (12)0.0234 (12)0.0116 (9)0.0036 (9)0.0021 (9)
C20.0339 (14)0.0280 (13)0.0354 (14)0.0153 (10)0.0046 (11)0.0063 (10)
C30.0324 (14)0.0292 (13)0.0294 (13)0.0110 (10)0.0003 (10)0.0084 (10)
C40.0270 (12)0.0244 (12)0.0242 (12)0.0094 (9)0.0046 (9)0.0016 (9)
C50.0238 (12)0.0250 (12)0.0234 (12)0.0078 (9)0.0033 (9)0.0027 (9)
C60.0257 (12)0.0314 (13)0.0233 (12)0.0104 (10)0.0018 (9)0.0049 (10)
C70.0273 (12)0.0273 (12)0.0240 (12)0.0077 (10)0.0021 (10)0.0040 (10)
C80.067 (2)0.0342 (15)0.0428 (17)0.0172 (14)0.0134 (15)0.0106 (13)
C90.0486 (18)0.0368 (16)0.0461 (17)0.0004 (13)0.0053 (14)0.0130 (13)
Geometric parameters (Å, º) top
Cu1—N11.994 (2)C1—C21.392 (4)
Cu1—N1i1.994 (2)C2—C31.378 (3)
Cu1—N2i2.009 (2)C2—H20.930
Cu1—N22.009 (2)C3—C41.395 (3)
S1—O31.445 (2)C3—H30.930
S1—O11.445 (2)C4—C51.396 (3)
S1—O21.4569 (19)C4—C7ii1.482 (3)
S1—C11.776 (2)C5—C61.394 (3)
O4—C71.216 (3)C5—C71.487 (3)
N1—C81.473 (4)C6—H60.930
N1—H1A0.900C7—C4ii1.482 (3)
N1—H1B0.900C8—C91.507 (4)
N2—C91.476 (3)C8—H8A0.970
N2—H2A0.900C8—H8B0.970
N2—H2B0.900C9—H9A0.970
C1—C61.384 (3)C9—H9B0.970
N1—Cu1—N1i180.0C1—C2—H2120.3
N1—Cu1—N2i94.83 (9)C2—C3—C4120.6 (2)
N1i—Cu1—N2i85.17 (9)C2—C3—H3119.7
N1—Cu1—N285.17 (9)C4—C3—H3119.7
N1i—Cu1—N294.83 (9)C3—C4—C5119.5 (2)
N2i—Cu1—N2180.0C3—C4—C7ii119.1 (2)
O3—S1—O1113.59 (13)C5—C4—C7ii121.3 (2)
O3—S1—O2112.45 (12)C6—C5—C4119.9 (2)
O1—S1—O2112.11 (13)C6—C5—C7118.7 (2)
O3—S1—C1105.75 (11)C4—C5—C7121.4 (2)
O1—S1—C1105.80 (12)C1—C6—C5119.6 (2)
O2—S1—C1106.42 (11)C1—C6—H6120.2
C8—N1—Cu1108.41 (17)C5—C6—H6120.2
C8—N1—H1A110.0O4—C7—C4ii121.5 (2)
Cu1—N1—H1A110.0O4—C7—C5121.1 (2)
C8—N1—H1B110.0C4ii—C7—C5117.3 (2)
Cu1—N1—H1B110.0N1—C8—C9107.7 (2)
H1A—N1—H1B108.4N1—C8—H8A110.2
C9—N2—Cu1107.83 (17)C9—C8—H8A110.2
C9—N2—H2A110.1N1—C8—H8B110.2
Cu1—N2—H2A110.1C9—C8—H8B110.2
C9—N2—H2B110.1H8A—C8—H8B108.5
Cu1—N2—H2B110.1N2—C9—C8107.3 (2)
H2A—N2—H2B108.5N2—C9—H9A110.2
C6—C1—C2120.8 (2)C8—C9—H9A110.2
C6—C1—S1119.33 (19)N2—C9—H9B110.2
C2—C1—S1119.87 (18)C8—C9—H9B110.2
C3—C2—C1119.5 (2)H9A—C9—H9B108.5
C3—C2—H2120.3
Symmetry codes: (i) x, y, z+1; (ii) x+2, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O3i0.902.122.922 (3)149
N1—H1B···O2iii0.902.353.172 (3)152
N2—H2A···O10.902.213.000 (3)146
N2—H2B···O2iv0.902.283.113 (3)154
Symmetry codes: (i) x, y, z+1; (iii) x+1, y, z+1; (iv) x1, y, z.
 

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.

Buy online

You may purchase this article in PDF and/or HTML formats. For purchasers in the European Community who do not have a VAT number, VAT will be added at the local rate. Payments to the IUCr are handled by WorldPay, who will accept payment by credit card in several currencies. To purchase the article, please complete the form below (fields marked * are required), and then click on `Continue'.
E-mail address* 
Repeat e-mail address* 
(for error checking) 

Format*   PDF (US $40)
   HTML (US $40)
   PDF+HTML (US $50)
In order for VAT to be shown for your country javascript needs to be enabled.

VAT number 
(non-UK EC countries only) 
Country* 
 

Terms and conditions of use
Contact us

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds