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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 4;67(Pt 7):m837–m838. doi: 10.1107/S1600536811019209

Poly[dimethyl­ammonium [aquadi-μ2-oxalato-yttriate(III)] trihydrate]

Yao-Kang Lv a, Li-Hua Gan a,*, Liang Xu a, Hao-Wen Zheng a, Cao Liu a
PMCID: PMC3151934  PMID: 21836844

Abstract

The title complex, {(C2H8N)[Y(C2O4)2(H2O)]·3H2O}n, was obtained accidentally under hydro­thermal conditions. The YIII atom is chelated by four oxalate ligands and one water mol­ecule resulting in a distorted tricapped trigonal–prismatic geometry. Each oxalate ligand bridges two YIII atoms, thus generating a three-dimensional network with cavities in which the ammonium cations and lattice water mol­ecules reside. Various O—H⋯O and N—H⋯O hydrogen-bonding inter­actions stabilize the crystal structure. The title complex is isotypic with the Eu and Dy analogues.

Related literature

For general background to the rational design and synthesis of metal-organic polymers, see: Lv et al. (2010, 2011). For related structures, see: Platel et al. (2009); Gao & Cui (2008); Deguenon et al. (1990). The structure of the isotypic EuIII compound was reported by Yang et al. (2005), and that of the DyIII compound by Ye & Lin (2010). For decomposition products obtained under hydro­thermal conditions, see: Song et al. (2004).graphic file with name e-67-0m837-scheme1.jpg

Experimental

Crystal data

  • (C2H8N)[Y(C2O4)2(H2O)]·3H2O

  • M r = 383.11

  • Monoclinic, Inline graphic

  • a = 9.6008 (1) Å

  • b = 11.5422 (2) Å

  • c = 14.2886 (2) Å

  • β = 122.460 (1)°

  • V = 1336.00 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 4.43 mm−1

  • T = 293 K

  • 0.31 × 0.20 × 0.19 mm

Data collection

  • Bruker APEXII area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.36, T max = 0.43

  • 11935 measured reflections

  • 3040 independent reflections

  • 2384 reflections with I > 2σ(I)

  • R int = 0.044

Refinement

  • R[F 2 > 2σ(F 2)] = 0.033

  • wR(F 2) = 0.082

  • S = 1.00

  • 3040 reflections

  • 207 parameters

  • 13 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.70 e Å−3

  • Δρmin = −0.58 e Å−3

Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2004); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811019209/wm2489sup1.cif

e-67-0m837-sup1.cif (20.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811019209/wm2489Isup2.hkl

e-67-0m837-Isup2.hkl (149.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1WA⋯O2Wi 0.83 (2) 1.93 (2) 2.742 (4) 167 (4)
O1W—H1WB⋯O2Wii 0.72 (2) 2.20 (2) 2.861 (4) 152 (4)
O2W—H2WA⋯O6iii 0.81 (2) 2.38 (2) 3.143 (4) 158 (5)
O2W—H2WA⋯O7iv 0.81 (2) 2.45 (5) 2.944 (4) 121 (5)
O2W—H2WB⋯O3Wv 0.79 (2) 2.38 (3) 2.963 (7) 131 (4)
O2W—H2WB⋯O4W 0.79 (2) 2.44 (3) 3.194 (6) 159 (5)
O3W—H3WA⋯O2 0.88 (2) 2.36 (7) 2.830 (5) 114 (6)
O3W—H3WB⋯O4Wiv 0.86 (2) 1.90 (3) 2.735 (6) 161 (6)
O4W—H4WA⋯O1vi 0.82 (2) 2.13 (2) 2.943 (4) 172 (5)
O4W—H4WB⋯O3vii 0.83 (2) 2.08 (3) 2.857 (4) 155 (6)
N1—H1A⋯O8vi 0.90 2.00 2.869 (4) 163
N1—H1A⋯O1Wvi 0.90 2.54 3.107 (4) 122
N1—H1B⋯O3W 0.90 1.90 2.784 (6) 166

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic; (vi) Inline graphic; (vii) Inline graphic.

Acknowledgments

The present work was supported financially by the National Natural Science Foundation of China (No. 20973127) and Shanghai Nanotechnology Promotion Center (No. 0952nm00800).

supplementary crystallographic information

Comment

Rational design and synthesis of metal-organic polymers have attracted much attention in the field of supramolecular chemistry and crystal engineering (Lv et al., 2010; 2011). Oxalate, which usually represent one of the products of the degradation of some organic compounds, is one of the simplest multidentate organic ligands potentially able to bridge metal ions in a bidentate chelating manner (Deguenon et al., 1990). Herein, we report the synthesis and structure of a novel yttrium(III) complex, (C2H8N)[Y(C2O4)2(H2O)].3H2O, (I).

Complex (I) is isotypic with its Eu(III) (Yang et al., 2005) and Dy(III) (Ye & Lin, 2010) analogues. As shown in Fig. 1, the YIII atom is chelated by four oxalate ligands and one water molecule resulting in a distorted tricapped trigonal-prismatic coordination environment. The Y—O bond lengths fall in the range of 2.374 (2)-2.459 (2) Å, which is in agreement with comparable values reported elsewhere (Platel et al., 2009; Gao & Cui, 2008). Each oxalate ligand bridges two YIII atoms, thus generating a three-dimensional network with cavities where the ammonium cations and lattice water molecules reside (Fig. 2). Furthermore, there are various hydrogen-bonding interactions (N—H···O and O—H···O), involving the lattice water molecules and the cations, which give rise to a tightly held network structure.

Experimental

A mixture of D-saccharic acid potassium salt (0.248 g, 1.0 mmol), Y(NO3)3.6H2O (0.191 g, 0.5 mmol) and N,N-dimethylformamide (20 ml) was stirred and heated at 373 K for 1 hour. The resulted colorless solution was kept at 293 K. Colorless block-shaped crystals of the title compound suitable for X-ray crystallographic study were obtained via slow evaporation within 2 weeks.

It is most likely that the oxalate ligands in this complex originates from the decomposition of the potassium salt of D-saccharic acid, and the protonated dimethylamine cations compensating the negative charge of the anionic network are believed to result from decomposition of the N,N-dimethylformamide solvent (Song et al., 2004; Ye & Lin, 2010).

Refinement

The hydrogen atoms attached to carbon and nitrogen atoms were positioned geometrically, while those attached to oxygen atom were located from difference Fourier maps. H atoms attached to C atoms were refined using a riding model with C—H = 0.96 Å and Uiso(H) = 1.2Ueq(C); H atoms attached to N atoms were refined with N—H = 0.90 Å and Uiso(H) = 1.2Ueq(N); H atoms attached to O atoms were refined without distance restraints and with Uiso(H) = 1.2Ueq(O).

Figures

Fig. 1.

Fig. 1.

An expanded vioew of the asymmetric unit of (I), showing the coordination of the YIII atom, and the presence of the lattice water molecules and the ammonium cation. All hydrogen atoms were omitted for clarity. [Symmetry codes: (i) -x + 1, y + 1/2, -z + 1/2; (ii) -x + 1, -y + 2, -z + 1; (iii) -x + 2, -y + 2, -z + 1.]

Fig. 2.

Fig. 2.

View of the three-dimensional framework of (I). All hydrogen atoms are omitted for clarity. Hydrogen bonding between donator and acceptor atoms is indicated by dashed lines.

Crystal data

(C2H8N)[Y(C2O4)2(H2O)]·3H2O F(000) = 776
Mr = 383.11 Dx = 1.905 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 2287 reflections
a = 9.6008 (1) Å θ = 2.0–28.0°
b = 11.5422 (2) Å µ = 4.43 mm1
c = 14.2886 (2) Å T = 293 K
β = 122.460 (1)° Block, colourless
V = 1336.00 (3) Å3 0.31 × 0.20 × 0.19 mm
Z = 4

Data collection

Bruker APEXII area-detector diffractometer 3040 independent reflections
Radiation source: fine-focus sealed tube 2384 reflections with I > 2σ(I)
graphite Rint = 0.044
ω scans θmax = 27.5°, θmin = 2.9°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −12→12
Tmin = 0.36, Tmax = 0.43 k = −14→14
11935 measured reflections l = −18→18

Refinement

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)] = 0.033 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.082 H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.0359P)2 + 1.2217P] where P = (Fo2 + 2Fc2)/3
3040 reflections (Δ/σ)max = 0.001
207 parameters Δρmax = 0.70 e Å3
13 restraints Δρmin = −0.58 e Å3

Special details

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)

x y z Uiso*/Ueq
Y1 0.61770 (3) 0.98846 (2) 0.33257 (2) 0.01817 (10)
O1 0.7049 (3) 0.78990 (17) 0.34286 (19) 0.0270 (5)
O2 0.6167 (3) 0.60733 (18) 0.2950 (2) 0.0304 (6)
O3 0.3054 (3) 0.68334 (17) 0.17013 (18) 0.0231 (5)
O4 0.3959 (3) 0.86535 (17) 0.20743 (19) 0.0259 (5)
O6 0.5198 (3) 0.88268 (18) 0.4319 (2) 0.0293 (5)
O7 0.5387 (3) 1.11238 (19) 0.4367 (2) 0.0320 (6)
O8 0.8892 (3) 0.99123 (17) 0.35640 (19) 0.0245 (5)
O9 0.8389 (3) 0.98964 (18) 0.52152 (19) 0.0278 (5)
O1W 0.6044 (3) 0.9808 (2) 0.1578 (2) 0.0348 (6)
H1WA 0.617 (5) 1.039 (2) 0.129 (3) 0.042*
H1WB 0.568 (4) 0.931 (2) 0.122 (3) 0.042*
O2W 1.3774 (5) 0.8468 (3) 0.9672 (3) 0.0649 (10)
H2WA 1.386 (6) 0.785 (3) 0.946 (4) 0.078*
H2WB 1.293 (4) 0.850 (4) 0.965 (5) 0.078*
O3W 0.8383 (7) 0.5082 (4) 0.5055 (4) 0.1038 (17)
H3WA 0.857 (10) 0.539 (5) 0.457 (5) 0.125*
H3WB 0.889 (8) 0.444 (3) 0.512 (6) 0.125*
O4W 1.0523 (5) 0.7844 (3) 0.9661 (3) 0.0861 (13)
H4WA 0.959 (3) 0.758 (5) 0.936 (4) 0.103*
H4WB 1.103 (6) 0.758 (5) 1.030 (2) 0.103*
N1 0.9245 (4) 0.6326 (3) 0.6962 (3) 0.0585 (11)
H1A 0.8928 0.6007 0.7394 0.070*
H1B 0.8808 0.5895 0.6341 0.070*
C1 0.5960 (4) 0.7148 (2) 0.2919 (3) 0.0222 (7)
C2 0.4163 (4) 0.7587 (2) 0.2166 (3) 0.0195 (6)
C3 0.4947 (4) 0.9335 (3) 0.4984 (3) 0.0243 (7)
C4 1.0151 (4) 1.0005 (2) 0.4524 (3) 0.0202 (6)
C5 1.0993 (6) 0.6253 (6) 0.7531 (5) 0.0864 (19)
H5A 1.1314 0.5459 0.7567 0.104*
H5B 1.1476 0.6553 0.8269 0.104*
H5C 1.1370 0.6699 0.7141 0.104*
C6 0.8547 (8) 0.7488 (5) 0.6652 (5) 0.0897 (19)
H6A 0.7365 0.7442 0.6254 0.108*
H6B 0.8872 0.7841 0.6190 0.108*
H6C 0.8944 0.7946 0.7309 0.108*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Y1 0.01775 (15) 0.01434 (15) 0.01968 (16) −0.00007 (11) 0.00824 (12) −0.00024 (11)
O1 0.0193 (12) 0.0194 (11) 0.0322 (14) −0.0013 (8) 0.0071 (11) −0.0044 (9)
O2 0.0264 (12) 0.0173 (11) 0.0332 (14) 0.0029 (9) 0.0066 (11) −0.0002 (9)
O3 0.0203 (11) 0.0193 (10) 0.0265 (13) −0.0017 (8) 0.0105 (10) −0.0016 (9)
O4 0.0232 (12) 0.0170 (10) 0.0285 (13) 0.0016 (8) 0.0079 (10) 0.0003 (9)
O6 0.0347 (13) 0.0252 (12) 0.0331 (15) −0.0039 (9) 0.0216 (12) −0.0047 (10)
O7 0.0424 (14) 0.0252 (12) 0.0402 (16) 0.0045 (10) 0.0301 (13) 0.0060 (10)
O8 0.0195 (10) 0.0307 (12) 0.0205 (11) 0.0009 (9) 0.0088 (9) −0.0019 (9)
O9 0.0209 (11) 0.0368 (13) 0.0265 (12) −0.0014 (9) 0.0132 (10) −0.0004 (10)
O1W 0.0408 (14) 0.0346 (14) 0.0265 (14) −0.0076 (12) 0.0165 (12) −0.0043 (11)
O2W 0.080 (3) 0.0390 (17) 0.069 (2) 0.0025 (16) 0.036 (2) 0.0072 (16)
O3W 0.112 (4) 0.095 (3) 0.061 (3) 0.031 (3) 0.017 (3) −0.013 (2)
O4W 0.070 (3) 0.061 (2) 0.069 (3) −0.0094 (19) −0.001 (2) 0.0154 (19)
N1 0.045 (2) 0.071 (3) 0.058 (3) −0.0039 (18) 0.027 (2) 0.022 (2)
C1 0.0233 (16) 0.0187 (15) 0.0242 (17) 0.0003 (11) 0.0124 (14) −0.0014 (12)
C2 0.0236 (17) 0.0206 (15) 0.0165 (16) −0.0012 (11) 0.0121 (14) −0.0026 (12)
C3 0.0184 (14) 0.0272 (17) 0.0257 (17) −0.0012 (12) 0.0108 (13) −0.0008 (13)
C4 0.0205 (14) 0.0145 (14) 0.0222 (16) 0.0004 (11) 0.0092 (13) −0.0013 (12)
C5 0.046 (3) 0.144 (6) 0.066 (4) −0.004 (3) 0.028 (3) 0.027 (4)
C6 0.110 (5) 0.073 (4) 0.103 (5) 0.024 (3) 0.068 (4) 0.029 (3)

Geometric parameters (Å, °)

Y1—O3i 2.374 (2) O2W—H2WA 0.805 (19)
Y1—O9 2.376 (2) O2W—H2WB 0.794 (19)
Y1—O4 2.380 (2) O3W—H3WA 0.88 (2)
Y1—O6 2.413 (2) O3W—H3WB 0.86 (2)
Y1—O1 2.417 (2) O4W—H4WA 0.82 (2)
Y1—O2i 2.422 (2) O4W—H4WB 0.83 (2)
Y1—O1W 2.432 (3) N1—C5 1.421 (6)
Y1—O8 2.441 (2) N1—C6 1.458 (6)
Y1—O7 2.459 (2) N1—H1A 0.9000
O1—C1 1.247 (3) N1—H1B 0.9000
O2—C1 1.254 (3) C1—C2 1.548 (4)
O2—Y1ii 2.422 (2) C3—O7iii 1.250 (4)
O3—C2 1.254 (3) C3—C3iii 1.536 (6)
O3—Y1ii 2.374 (2) C4—O9iv 1.248 (4)
O4—C2 1.243 (3) C4—C4iv 1.535 (6)
O6—C3 1.246 (4) C5—H5A 0.9600
O7—C3iii 1.250 (4) C5—H5B 0.9600
O8—C4 1.255 (4) C5—H5C 0.9600
O9—C4iv 1.248 (4) C6—H6A 0.9600
O1W—H1WA 0.828 (18) C6—H6B 0.9600
O1W—H1WB 0.720 (17) C6—H6C 0.9600
O3i—Y1—O9 85.24 (7) C3—O6—Y1 120.4 (2)
O3i—Y1—O4 135.57 (7) C3iii—O7—Y1 119.2 (2)
O9—Y1—O4 138.66 (8) C4—O8—Y1 118.9 (2)
O3i—Y1—O6 135.37 (8) C4iv—O9—Y1 121.0 (2)
O9—Y1—O6 74.17 (8) Y1—O1W—H1WA 122 (3)
O4—Y1—O6 70.48 (8) Y1—O1W—H1WB 119 (3)
O3i—Y1—O1 143.01 (7) H1WA—O1W—H1WB 117 (3)
O9—Y1—O1 82.37 (7) H2WA—O2W—H2WB 110 (3)
O4—Y1—O1 67.70 (7) H3WA—O3W—H3WB 95 (7)
O6—Y1—O1 73.50 (8) H4WA—O4W—H4WB 106 (3)
O3i—Y1—O2i 67.82 (7) C5—N1—C6 115.9 (5)
O9—Y1—O2i 139.01 (8) C5—N1—H1A 108.3
O4—Y1—O2i 71.18 (7) C6—N1—H1A 108.3
O6—Y1—O2i 103.39 (8) C5—N1—H1B 108.3
O1—Y1—O2i 137.25 (7) C6—N1—H1B 108.3
O3i—Y1—O1W 82.13 (8) H1A—N1—H1B 107.4
O9—Y1—O1W 133.57 (8) O1—C1—O2 126.8 (3)
O4—Y1—O1W 70.99 (8) O1—C1—C2 116.8 (2)
O6—Y1—O1W 139.75 (8) O2—C1—C2 116.4 (3)
O1—Y1—O1W 81.59 (8) O4—C2—O3 126.2 (3)
O2i—Y1—O1W 74.46 (9) O4—C2—C1 116.8 (3)
O3i—Y1—O8 70.84 (7) O3—C2—C1 117.0 (3)
O9—Y1—O8 66.75 (7) O6—C3—O7iii 126.7 (3)
O4—Y1—O8 124.78 (8) O6—C3—C3iii 117.1 (4)
O6—Y1—O8 130.44 (8) O7iii—C3—C3iii 116.2 (4)
O1—Y1—O8 72.24 (7) O9iv—C4—O8 127.1 (3)
O2i—Y1—O8 126.06 (8) O9iv—C4—C4iv 116.9 (3)
O1W—Y1—O8 66.89 (8) O8—C4—C4iv 116.0 (3)
O3i—Y1—O7 70.02 (7) N1—C5—H5A 109.5
O9—Y1—O7 71.75 (8) N1—C5—H5B 109.5
O4—Y1—O7 111.09 (8) H5A—C5—H5B 109.5
O6—Y1—O7 66.06 (8) N1—C5—H5C 109.5
O1—Y1—O7 136.38 (8) H5A—C5—H5C 109.5
O2i—Y1—O7 70.27 (8) H5B—C5—H5C 109.5
O1W—Y1—O7 141.16 (8) N1—C6—H6A 109.5
O8—Y1—O7 124.12 (8) N1—C6—H6B 109.5
C1—O1—Y1 117.95 (18) H6A—C6—H6B 109.5
C1—O2—Y1ii 117.94 (19) N1—C6—H6C 109.5
C2—O3—Y1ii 118.85 (19) H6A—C6—H6C 109.5
C2—O4—Y1 119.03 (19) H6B—C6—H6C 109.5
O3i—Y1—O1—C1 −146.8 (2) O3i—Y1—O8—C4 87.9 (2)
O9—Y1—O1—C1 141.7 (2) O9—Y1—O8—C4 −5.14 (19)
O4—Y1—O1—C1 −9.2 (2) O4—Y1—O8—C4 −139.29 (19)
O6—Y1—O1—C1 66.0 (2) O6—Y1—O8—C4 −46.0 (2)
O2i—Y1—O1—C1 −26.0 (3) O1—Y1—O8—C4 −94.3 (2)
O1W—Y1—O1—C1 −82.0 (2) O2i—Y1—O8—C4 129.6 (2)
O8—Y1—O1—C1 −150.3 (3) O1W—Y1—O8—C4 177.4 (2)
O7—Y1—O1—C1 88.5 (3) O7—Y1—O8—C4 40.2 (2)
O3i—Y1—O4—C2 156.4 (2) O3i—Y1—O9—C4iv −65.9 (2)
O9—Y1—O4—C2 −35.0 (3) O4—Y1—O9—C4iv 122.1 (2)
O6—Y1—O4—C2 −67.7 (2) O6—Y1—O9—C4iv 154.1 (2)
O1—Y1—O4—C2 11.9 (2) O1—Y1—O9—C4iv 79.1 (2)
O2i—Y1—O4—C2 179.9 (3) O2i—Y1—O9—C4iv −113.6 (2)
O1W—Y1—O4—C2 100.4 (2) O1W—Y1—O9—C4iv 8.5 (3)
O8—Y1—O4—C2 58.5 (3) O8—Y1—O9—C4iv 5.23 (19)
O7—Y1—O4—C2 −121.0 (2) O7—Y1—O9—C4iv −136.5 (2)
O3i—Y1—O6—C3 2.2 (3) Y1—O1—C1—O2 −173.7 (3)
O9—Y1—O6—C3 68.0 (2) Y1—O1—C1—C2 6.4 (4)
O4—Y1—O6—C3 −133.8 (3) Y1ii—O2—C1—O1 −172.3 (3)
O1—Y1—O6—C3 154.5 (3) Y1ii—O2—C1—C2 7.6 (4)
O2i—Y1—O6—C3 −69.7 (2) Y1—O4—C2—O3 167.4 (2)
O1W—Y1—O6—C3 −151.3 (2) Y1—O4—C2—C1 −13.2 (4)
O8—Y1—O6—C3 106.6 (2) Y1ii—O3—C2—O4 165.7 (3)
O7—Y1—O6—C3 −8.7 (2) Y1ii—O3—C2—C1 −13.8 (4)
O3i—Y1—O7—C3iii −163.4 (3) O1—C1—C2—O4 4.4 (4)
O9—Y1—O7—C3iii −71.8 (2) O2—C1—C2—O4 −175.5 (3)
O4—Y1—O7—C3iii 64.3 (3) O1—C1—C2—O3 −176.1 (3)
O6—Y1—O7—C3iii 8.5 (2) O2—C1—C2—O3 4.0 (4)
O1—Y1—O7—C3iii −15.1 (3) Y1—O6—C3—O7iii −171.9 (3)
O2i—Y1—O7—C3iii 123.9 (3) Y1—O6—C3—C3iii 8.3 (5)
O1W—Y1—O7—C3iii 149.8 (2) Y1—O8—C4—O9iv −175.3 (2)
O8—Y1—O7—C3iii −115.3 (2) Y1—O8—C4—C4iv 4.7 (4)

Symmetry codes: (i) −x+1, y+1/2, −z+1/2; (ii) −x+1, y−1/2, −z+1/2; (iii) −x+1, −y+2, −z+1; (iv) −x+2, −y+2, −z+1.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—H1WA···O2Wiv 0.83 (2) 1.93 (2) 2.742 (4) 167 (4)
O1W—H1WB···O2Wv 0.72 (2) 2.20 (2) 2.861 (4) 152 (4)
O2W—H2WA···O6vi 0.81 (2) 2.38 (2) 3.143 (4) 158 (5)
O2W—H2WA···O7vii 0.81 (2) 2.45 (5) 2.944 (4) 121 (5)
O2W—H2WB···O3Wviii 0.79 (2) 2.38 (3) 2.963 (7) 131 (4)
O2W—H2WB···O4W 0.79 (2) 2.44 (3) 3.194 (6) 159 (5)
O3W—H3WA···O2 0.88 (2) 2.36 (7) 2.830 (5) 114 (6)
O3W—H3WB···O4Wvii 0.86 (2) 1.90 (3) 2.735 (6) 161 (6)
O4W—H4WA···O1ix 0.82 (2) 2.13 (2) 2.943 (4) 172 (5)
O4W—H4WB···O3x 0.83 (2) 2.08 (3) 2.857 (4) 155 (6)
N1—H1A···O8ix 0.90 2.00 2.869 (4) 163
N1—H1A···O1Wix 0.90 2.54 3.107 (4) 122
N1—H1B···O3W 0.90 1.90 2.784 (6) 166

Symmetry codes: (iv) −x+2, −y+2, −z+1; (v) x−1, y, z−1; (vi) x+1, −y+3/2, z+1/2; (vii) −x+2, y−1/2, −z+3/2; (viii) −x+2, y+1/2, −z+3/2; (ix) x, −y+3/2, z+1/2; (x) x+1, y, z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2489).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811019209/wm2489sup1.cif

e-67-0m837-sup1.cif (20.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811019209/wm2489Isup2.hkl

e-67-0m837-Isup2.hkl (149.2KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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