Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 7;67(Pt 5):m529–m530. doi: 10.1107/S1600536811011251

Yttrium ethyl­enediammonium squarate tetra­hydrate

Louiza Zenkhri a,*, Nathalie Audebrand b, Thierry Bataille b
PMCID: PMC3089218  PMID: 21754270

Abstract

The title compound, {(C2H10N2)1.5[Y(C4O4)3(H2O)4]}n {system­atic name: catena-poly[sesqui(ethyl­enediammonium) [[tetra­aquabis­(squarato-κO)yttrium(III)]-μ-squarato-κ2 O:O′]]}, was synthesized by slow evaporation of an acid solution. The asymetric unit contains one yttrium cation in an anti­prismatic environnement, three squarate groups, one and a half protonated ethyl­enediamine mol­ecules and four water mol­ecules. YO8 polyhedra are connected through bis­(mono­dentate) squarates, leading to infinite zigzag chains, in between which are located ammonium groups. A framework of hydrogen bonds between protonated amine N atoms, water mol­ecules and squarate anions ensures the cohesion of the structure.

Related literature

For a related structure, see: Kazerouni et al. (1994) ▶. The title compound was obtained together with two polymorphs of (C2H10N2)(HC4O4)2(H2O) (Mathew et al., 2002 ▶; Zenkhri et al., 2011) ▶. For related yttrium squarates with potassium, see: Mahé & Bataille (2004 ▶).graphic file with name e-67-0m529-scheme1.jpg

Experimental

Crystal data

  • (C2H10N2)1.5[Y(C4O4)3(H2O)4]

  • M r = 590.27

  • Monoclinic, Inline graphic

  • a = 8.9780 (2) Å

  • b = 13.2864 (3) Å

  • c = 18.3970 (4) Å

  • β = 90.935 (1)°

  • V = 2194.20 (8) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.75 mm−1

  • T = 293 K

  • 0.22 × 0.14 × 0.12 mm

Data collection

  • Nonius KappaCCD diffractometer

  • Absorption correction: analytical (de Meulenaer & Tompa, 1965) ▶ T min = 0.583, T max = 0.734

  • 23285 measured reflections

  • 5016 independent reflections

  • 4140 reflections with I > 2σ(I)

  • R int = 0.065

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.103

  • S = 1.10

  • 5016 reflections

  • 316 parameters

  • H-atom parameters constrained

  • Δρmax = 1.77 e Å−3

  • Δρmin = −0.62 e Å−3

Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: DIRAX/LSQ (Duisenberg, 1992 ▶); data reduction: EVALCCD (Duisenberg et al., 2003 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Berndt, 2001 ▶); software used to prepare material for publication: WinGX publication routines (Farrugia, 1999 ▶).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811011251/ru2003sup1.cif

e-67-0m529-sup1.cif (30.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011251/ru2003Isup2.hkl

e-67-0m529-Isup2.hkl (240.7KB, hkl)

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

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

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N1—H12⋯O3i 0.87 2.21 3.027 (4) 157
N1—H12⋯O9ii 0.87 2.36 2.929 (4) 123
N1—H11⋯O4i 0.87 2.36 2.995 (4) 131
N1—H11⋯O7ii 0.87 2.28 2.987 (4) 138
N1—H13⋯O6ii 0.87 2.36 2.970 (4) 127
N1—H13⋯O12ii 0.87 2.26 3.032 (4) 148
N2—H23⋯O2 0.85 1.87 2.707 (4) 167
N2—H21⋯O4i 0.96 1.92 2.832 (4) 159
N2—H21⋯O7ii 0.96 2.46 2.952 (4) 112
N2—H22⋯O5iii 0.95 2.01 2.929 (4) 163
N3—H31⋯O4 0.87 2.22 2.843 (4) 129
N3—H32⋯O8iv 0.87 2.18 2.788 (4) 127
N3—H33⋯OW1v 0.87 2.40 2.997 (4) 126
OW1—H911⋯O11v 0.94 1.74 2.676 (3) 175
OW1—H912⋯O5 0.93 1.78 2.687 (3) 166
OW2—H922⋯O11 0.94 1.95 2.885 (4) 173
OW2—H921⋯O10v 0.94 1.79 2.726 (3) 179
OW3—H931⋯O8vi 0.93 1.94 2.857 (4) 172
OW3—H932⋯O1i 0.94 2.04 2.954 (5) 163
OW4—H942⋯O5vi 0.92 1.86 2.779 (3) 172
OW4—H941⋯O10vii 0.93 1.86 2.761 (4) 163

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

Acknowledgments

Grateful thanks are expressed to Dr T. Roisnel (Centre de Diffractométrie X, UMR CNRS 6226) for his assistance with the data collection.

supplementary crystallographic information

Comment

In the course of a study on mixed squarate of amines and metals, the role of the amine group has been investigated in the topology of the organic-inorganic framework. The synthesis led to a new mixed squarate of yttrium and ethylenediamine.

Yttrium is eightfold coordinated in the shape of a square antiprism. YO8 polyhedra are connected along the b axis through bis(monodentate) squarates in the form of zigzag chains (Figures 1, 2). Amine groups are located between the chains (Figure 2) and are connected to them through hydrogen bonds involving oxygen atoms from squarate groups (Table 1). Other hydrogen bonds between water molecules and squarate groups contribute also to the formation of a three-dimensional molecular framework (Table 1). One ethylenediammonium possesses a gauche conformation as already reported for this molecule (Kazerouni et al., 1994).

Experimental

The title compound, Y(C4O4)3(C2H10N2)1.54H2O was prepared from an aquous solution (20 ml) of dissolved yttrium nitrate (0.5 mmol), ethylenediamine (0.1 mmol) and 3,4-dihydroxy-3-cyclobutene-1,2-dione, also named squaric acid (0.1 mmol). The slow evaporation at room temperature leads after some hours to the formation of the title compound together with two polymorphs of (HC4O4)2(C2H10N2)(H2O) (Mathew et al., 2002; Zenkhri et al.., 2011).

Refinement

All H atoms were found from Fourier difference maps. H atoms attached to C were fixed geometrically and treated as riding with C—H = 0.97 Å with Uiso(H) = 1.2Ueq. As H atoms attached to N and O are not geometrically tightened, they were refined using restraints of N–H = 0.89 (1)Å and O–H = 0.97 (1)Å with Uiso(H) = 1.2Ueq(N) and Uiso(H) = 1.5Ueq(O), respectively. In the last cycles of refinement, they were treated as riding on their parent atoms.

Figures

Fig. 1.

Fig. 1.

View of the molecular structure of the title compound. Ellipsoids are shown at the 50% probability level. (i) 1 - x, -1 - y, 2 - z; (ii) 2 - x, -1/2 + y, 3/2 - z.

Fig. 2.

Fig. 2.

View of the structure of the title compound along the a axis displaying chains alternating with amine groups.

Crystal data

(C2H10N2)1.5[Y(C4O4)3(H2O)4] F(000) = 1204
Mr = 590.27 Dx = 1.787 Mg m−3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
a = 8.9780 (2) Å Cell parameters from 57148 reflections
b = 13.2864 (3) Å θ = 2.9–27.5°
c = 18.3970 (4) Å µ = 2.75 mm−1
β = 90.935 (1)° T = 293 K
V = 2194.20 (8) Å3 Prism, colourless
Z = 4 0.22 × 0.14 × 0.12 mm

Data collection

Nonius KappaCCD diffractometer 5016 independent reflections
Radiation source: fine-focus sealed tube 4140 reflections with I > 2σ(I)
horizonally mounted graphite crystal Rint = 0.065
Detector resolution: 9 pixels mm-1 θmax = 27.5°, θmin = 2.9°
CCD scans h = −11→11
Absorption correction: analytical (de Meulenaer & Tompa, 1965) k = −17→17
Tmin = 0.583, Tmax = 0.734 l = −23→23
23285 measured reflections

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)] = 0.041 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103 H-atom parameters constrained
S = 1.10 w = 1/[σ2(Fo2) + (0.0368P)2 + 4.9093P] where P = (Fo2 + 2Fc2)/3
5016 reflections (Δ/σ)max = 0.002
316 parameters Δρmax = 1.77 e Å−3
0 restraints Δρmin = −0.62 e Å−3

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 > 2σ(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 0.81967 (3) 0.09385 (2) 0.775395 (16) 0.01739 (9)
OW1 0.6982 (2) −0.02399 (18) 0.69447 (13) 0.0255 (5)
H911 0.6156 −0.0626 0.7085 0.038*
H912 0.7647 −0.0720 0.6785 0.038*
OW2 0.5760 (3) 0.15385 (18) 0.74497 (16) 0.0332 (6)
H921 0.4774 0.1303 0.7446 0.050*
H922 0.5568 0.2216 0.7550 0.050*
OW3 0.7609 (4) 0.1825 (2) 0.88343 (19) 0.0653 (12)
H931 0.7880 0.2376 0.9116 0.098*
H932 0.7345 0.1447 0.9243 0.098*
OW4 1.0544 (3) 0.16009 (19) 0.82212 (15) 0.0332 (6)
H941 1.1451 0.1438 0.8013 0.050*
H942 1.0623 0.2267 0.8356 0.050*
C1 0.3965 (4) −0.0751 (3) 0.9370 (2) 0.0344 (9)
O1 0.2824 (3) −0.0919 (3) 0.97182 (19) 0.0618 (10)
C2 0.4625 (4) 0.0166 (3) 0.90558 (19) 0.0308 (8)
O2 0.4298 (4) 0.1078 (2) 0.90299 (18) 0.0567 (9)
C3 0.5884 (4) −0.0427 (2) 0.88126 (17) 0.0215 (6)
O3 0.7096 (2) −0.02378 (17) 0.84855 (13) 0.0260 (5)
C4 0.5259 (4) −0.1337 (3) 0.91110 (19) 0.0270 (7)
O4 0.5696 (3) −0.2235 (2) 0.91517 (16) 0.0389 (6)
C5 0.9863 (4) −0.0763 (2) 0.60978 (17) 0.0212 (6)
O5 0.8971 (3) −0.14412 (17) 0.62986 (14) 0.0283 (5)
C6 1.0043 (4) 0.0306 (2) 0.62387 (17) 0.0212 (6)
O6 0.9443 (3) 0.09575 (17) 0.66401 (13) 0.0278 (5)
C7 1.1316 (4) 0.0349 (2) 0.57414 (18) 0.0228 (6)
O7 1.2148 (3) 0.10214 (18) 0.55251 (16) 0.0356 (6)
C8 1.1158 (4) −0.0751 (2) 0.56315 (18) 0.0227 (7)
O8 1.1858 (3) −0.14202 (19) 0.53033 (16) 0.0368 (6)
C9 0.8814 (3) 0.4399 (2) 0.72880 (17) 0.0190 (6)
O9 1.0131 (2) 0.46219 (16) 0.71244 (13) 0.0244 (5)
C10 0.7446 (4) 0.4939 (2) 0.74815 (18) 0.0225 (6)
O10 0.7095 (3) 0.58392 (18) 0.75490 (17) 0.0360 (6)
C11 0.6683 (3) 0.3960 (2) 0.75669 (18) 0.0216 (6)
O11 0.5417 (3) 0.3661 (2) 0.77318 (16) 0.0351 (6)
C12 0.8066 (3) 0.3451 (2) 0.73838 (17) 0.0203 (6)
O12 0.8488 (3) 0.25554 (17) 0.73267 (15) 0.0316 (6)
N1 0.1150 (3) 0.2173 (2) 1.13530 (16) 0.0276 (6)
H11 0.1863 0.2579 1.1230 0.033*
H12 0.1531 0.1615 1.1520 0.033*
H13 0.0618 0.2454 1.1688 0.033*
C13 0.0190 (4) 0.1952 (3) 1.0706 (2) 0.0315 (8)
H131 −0.0192 0.2581 1.0511 0.038*
H132 −0.0654 0.1553 1.0858 0.038*
C14 0.0985 (4) 0.1398 (3) 1.0114 (2) 0.0317 (8)
H141 0.1488 0.0817 1.0323 0.038*
H142 0.0257 0.1156 0.9760 0.038*
N2 0.2096 (3) 0.2041 (2) 0.97398 (16) 0.0300 (7)
H21 0.2778 0.2278 1.0107 0.036*
H22 0.1607 0.2561 0.9477 0.036*
H23 0.2683 0.1717 0.9464 0.036*
N3 0.4125 (4) −0.4070 (3) 0.93482 (18) 0.0392 (8)
H31 0.4774 −0.3779 0.9072 0.047*
H32 0.3940 −0.3685 0.9718 0.047*
H33 0.3306 −0.4175 0.9100 0.047*
C15 0.4730 (4) −0.5043 (3) 0.9610 (2) 0.0348 (9)
H151 0.5550 −0.5246 0.9306 0.042*
H152 0.3963 −0.5555 0.9574 0.042*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Y1 0.01584 (14) 0.01229 (13) 0.02423 (15) 0.00006 (11) 0.00636 (10) 0.00037 (12)
OW1 0.0212 (11) 0.0241 (12) 0.0313 (12) −0.0036 (9) 0.0061 (9) −0.0030 (10)
OW2 0.0161 (11) 0.0211 (12) 0.0625 (18) 0.0014 (9) 0.0049 (11) 0.0036 (12)
OW3 0.099 (3) 0.0388 (17) 0.060 (2) −0.0325 (18) 0.055 (2) −0.0255 (15)
OW4 0.0302 (13) 0.0235 (12) 0.0456 (16) −0.0003 (10) −0.0048 (11) −0.0100 (11)
C1 0.0197 (16) 0.058 (3) 0.0259 (18) −0.0034 (16) 0.0021 (13) 0.0039 (16)
O1 0.0269 (15) 0.104 (3) 0.055 (2) −0.0107 (17) 0.0177 (14) 0.011 (2)
C2 0.0284 (18) 0.042 (2) 0.0228 (17) 0.0099 (16) 0.0066 (14) 0.0032 (15)
O2 0.068 (2) 0.0505 (19) 0.0524 (19) 0.0358 (17) 0.0266 (17) 0.0089 (15)
C3 0.0219 (15) 0.0236 (16) 0.0190 (15) 0.0011 (13) 0.0032 (12) 0.0002 (12)
O3 0.0234 (11) 0.0234 (12) 0.0317 (13) 0.0022 (9) 0.0116 (10) 0.0058 (10)
C4 0.0217 (16) 0.0335 (18) 0.0257 (17) −0.0081 (14) −0.0004 (13) 0.0042 (14)
O4 0.0408 (15) 0.0259 (13) 0.0498 (17) −0.0086 (12) 0.0008 (13) 0.0090 (12)
C5 0.0258 (16) 0.0155 (14) 0.0224 (15) 0.0002 (12) 0.0017 (12) 0.0011 (11)
O5 0.0297 (12) 0.0183 (11) 0.0373 (14) −0.0060 (10) 0.0110 (10) −0.0002 (10)
C6 0.0249 (15) 0.0158 (14) 0.0232 (16) −0.0003 (12) 0.0055 (12) 0.0006 (12)
O6 0.0352 (13) 0.0170 (11) 0.0317 (13) −0.0019 (10) 0.0166 (10) −0.0012 (10)
C7 0.0238 (16) 0.0182 (15) 0.0265 (16) 0.0022 (12) 0.0068 (13) 0.0024 (12)
O7 0.0364 (14) 0.0196 (12) 0.0517 (16) −0.0027 (11) 0.0238 (12) 0.0033 (11)
C8 0.0243 (16) 0.0182 (15) 0.0258 (16) 0.0005 (12) 0.0025 (13) −0.0006 (12)
O8 0.0382 (14) 0.0227 (13) 0.0500 (17) 0.0037 (11) 0.0193 (12) −0.0081 (11)
C9 0.0183 (14) 0.0160 (14) 0.0229 (15) 0.0008 (11) 0.0034 (12) −0.0004 (12)
O9 0.0177 (11) 0.0168 (11) 0.0390 (14) −0.0030 (9) 0.0086 (9) −0.0019 (10)
C10 0.0195 (15) 0.0193 (15) 0.0289 (17) 0.0032 (12) 0.0023 (12) −0.0001 (13)
O10 0.0253 (12) 0.0161 (12) 0.0668 (19) 0.0064 (10) 0.0064 (12) −0.0027 (12)
C11 0.0174 (14) 0.0193 (15) 0.0282 (16) 0.0020 (12) 0.0045 (12) 0.0017 (13)
O11 0.0181 (11) 0.0275 (13) 0.0602 (18) 0.0025 (10) 0.0131 (11) 0.0071 (12)
C12 0.0185 (14) 0.0177 (14) 0.0247 (16) 0.0015 (12) 0.0040 (12) 0.0036 (12)
O12 0.0275 (12) 0.0132 (11) 0.0546 (16) 0.0009 (9) 0.0149 (11) 0.0046 (11)
N1 0.0320 (15) 0.0198 (13) 0.0314 (16) 0.0027 (12) 0.0110 (12) 0.0010 (12)
C13 0.0216 (16) 0.0338 (19) 0.039 (2) 0.0014 (14) 0.0029 (14) 0.0051 (16)
C14 0.040 (2) 0.0239 (17) 0.0309 (19) 0.0005 (15) −0.0044 (15) 0.0000 (14)
N2 0.0353 (16) 0.0283 (15) 0.0267 (15) 0.0109 (13) 0.0061 (12) −0.0009 (12)
N3 0.0367 (18) 0.046 (2) 0.0351 (17) −0.0108 (16) 0.0085 (14) −0.0034 (15)
C15 0.0296 (18) 0.044 (2) 0.031 (2) −0.0111 (16) 0.0079 (15) −0.0092 (16)

Geometric parameters (Å, °)

Y1—O3 2.297 (2) C8—O8 1.250 (4)
Y1—O12 2.304 (2) C9—O9 1.261 (4)
Y1—O9i 2.314 (2) C9—C12 1.439 (4)
Y1—O6 2.351 (2) C9—C10 1.471 (4)
Y1—OW3 2.377 (3) O9—Y1ii 2.314 (2)
Y1—OW2 2.386 (2) C10—O10 1.244 (4)
Y1—OW1 2.409 (2) C10—C11 1.479 (4)
Y1—OW4 2.428 (2) C11—O11 1.247 (4)
OW1—H911 0.9405 C11—C12 1.458 (4)
OW1—H912 0.9255 C12—O12 1.254 (4)
OW2—H921 0.9388 N1—C13 1.487 (5)
OW2—H922 0.9354 N1—H11 0.8700
OW3—H931 0.9277 N1—H12 0.8700
OW3—H932 0.9382 N1—H13 0.8700
OW4—H941 0.9307 C13—C14 1.504 (5)
OW4—H942 0.9214 C13—H131 0.9700
C1—O1 1.237 (4) C13—H132 0.9700
C1—C2 1.476 (5) C14—N2 1.491 (5)
C1—C4 1.484 (5) C14—H141 0.9700
C2—O2 1.249 (5) C14—H142 0.9700
C2—C3 1.454 (5) N2—H21 0.9571
C3—O3 1.277 (4) N2—H22 0.9479
C3—C4 1.445 (5) N2—H23 0.8528
C4—O4 1.257 (5) N3—C15 1.479 (5)
C5—O5 1.265 (4) N3—H31 0.8700
C5—C6 1.453 (4) N3—H32 0.8700
C5—C8 1.456 (4) N3—H33 0.8700
C6—O6 1.264 (4) C15—C15iii 1.512 (8)
C6—C7 1.476 (4) C15—H151 0.9700
C7—O7 1.234 (4) C15—H152 0.9700
C7—C8 1.482 (4)
O3—Y1—O12 152.48 (8) C5—C6—C7 90.7 (3)
O3—Y1—O9i 73.35 (8) C6—O6—Y1 135.7 (2)
O12—Y1—O9i 131.37 (8) O7—C7—C6 134.9 (3)
O3—Y1—O6 137.19 (8) O7—C7—C8 136.6 (3)
O12—Y1—O6 68.55 (8) C6—C7—C8 88.4 (2)
O9i—Y1—O6 77.00 (8) O8—C8—C5 133.6 (3)
O3—Y1—OW3 75.14 (9) O8—C8—C7 136.0 (3)
O12—Y1—OW3 81.46 (10) C5—C8—C7 90.3 (2)
O9i—Y1—OW3 116.50 (12) O9—C9—C12 132.6 (3)
O6—Y1—OW3 147.03 (9) O9—C9—C10 137.1 (3)
O3—Y1—OW2 87.89 (8) C12—C9—C10 90.2 (2)
O12—Y1—OW2 73.57 (8) C9—O9—Y1ii 139.9 (2)
O9i—Y1—OW2 150.02 (8) O10—C10—C9 135.0 (3)
O6—Y1—OW2 103.86 (9) O10—C10—C11 135.7 (3)
OW3—Y1—OW2 79.37 (13) C9—C10—C11 89.2 (2)
O3—Y1—OW1 74.04 (8) O11—C11—C12 133.8 (3)
O12—Y1—OW1 116.61 (9) O11—C11—C10 137.0 (3)
O9i—Y1—OW1 81.66 (8) C12—C11—C10 89.2 (2)
O6—Y1—OW1 71.68 (8) O12—C12—C9 132.7 (3)
OW3—Y1—OW1 137.23 (10) O12—C12—C11 135.9 (3)
OW2—Y1—OW1 70.61 (9) C9—C12—C11 91.4 (2)
O3—Y1—OW4 114.74 (9) C12—O12—Y1 145.1 (2)
O12—Y1—OW4 71.35 (9) C13—N1—H11 109.5
O9i—Y1—OW4 71.44 (8) C13—N1—H12 109.5
O6—Y1—OW4 83.21 (9) H11—N1—H12 109.5
OW3—Y1—OW4 74.20 (11) C13—N1—H13 109.5
OW2—Y1—OW4 138.51 (9) H11—N1—H13 109.5
OW1—Y1—OW4 146.71 (8) H12—N1—H13 109.5
Y1—OW1—H911 122.4 N1—C13—C14 113.6 (3)
Y1—OW1—H912 110.8 N1—C13—H131 108.8
H911—OW1—H912 103.1 C14—C13—H131 108.8
Y1—OW2—H921 138.7 N1—C13—H132 108.8
Y1—OW2—H922 116.5 C14—C13—H132 108.8
H921—OW2—H922 98.3 H131—C13—H132 107.7
Y1—OW3—H931 142.9 N2—C14—C13 112.5 (3)
Y1—OW3—H932 117.9 N2—C14—H141 109.1
H931—OW3—H932 92.4 C13—C14—H141 109.1
Y1—OW4—H941 122.0 N2—C14—H142 109.1
Y1—OW4—H942 120.4 C13—C14—H142 109.1
H941—OW4—H942 105.7 H141—C14—H142 107.8
O1—C1—C2 133.9 (4) C14—N2—H21 106.7
O1—C1—C4 136.9 (4) C14—N2—H22 110.2
C2—C1—C4 89.2 (3) H21—N2—H22 113.9
O2—C2—C3 134.3 (4) C14—N2—H23 114.2
O2—C2—C1 136.1 (3) H21—N2—H23 101.0
C3—C2—C1 89.6 (3) H22—N2—H23 110.5
O3—C3—C4 133.1 (3) C15—N3—H31 109.5
O3—C3—C2 135.3 (3) C15—N3—H32 109.5
C4—C3—C2 91.6 (3) H31—N3—H32 109.5
C3—O3—Y1 142.0 (2) C15—N3—H33 109.5
O4—C4—C3 133.9 (3) H31—N3—H33 109.5
O4—C4—C1 136.4 (3) H32—N3—H33 109.5
C3—C4—C1 89.6 (3) N3—C15—C15iii 110.7 (4)
O5—C5—C6 135.6 (3) N3—C15—H151 109.5
O5—C5—C8 134.0 (3) C15iii—C15—H151 109.5
C6—C5—C8 90.4 (2) N3—C15—H152 109.5
O6—C6—C5 136.6 (3) C15iii—C15—H152 109.5
O6—C6—C7 132.6 (3) H151—C15—H152 108.1

Symmetry codes: (i) −x+2, y−1/2, −z+3/2; (ii) −x+2, y+1/2, −z+3/2; (iii) −x+1, −y−1, −z+2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H12···O3iv 0.87 2.21 3.027 (4) 157
N1—H12···O9v 0.87 2.36 2.929 (4) 123
N1—H11···O4iv 0.87 2.36 2.995 (4) 131
N1—H11···O7v 0.87 2.28 2.987 (4) 138
N1—H13···O6v 0.87 2.36 2.970 (4) 127
N1—H13···O12v 0.87 2.26 3.032 (4) 148
N2—H23···O2 0.85 1.87 2.707 (4) 167
N2—H21···O4iv 0.96 1.92 2.832 (4) 159
N2—H21···O7v 0.96 2.46 2.952 (4) 112
N2—H22···O5vi 0.95 2.01 2.929 (4) 163
N3—H31···O4 0.87 2.22 2.843 (4) 129
N3—H32···O8vii 0.87 2.18 2.788 (4) 127
N3—H33···OW1viii 0.87 2.40 2.997 (4) 126
OW1—H911···O11viii 0.94 1.74 2.676 (3) 175
OW1—H912···O5 0.93 1.78 2.687 (3) 166
OW2—H922···O11 0.94 1.95 2.885 (4) 173
OW2—H921···O10viii 0.94 1.79 2.726 (3) 179
OW3—H931···O8ii 0.93 1.94 2.857 (4) 172
OW3—H932···O1iv 0.94 2.04 2.954 (5) 163
OW4—H942···O5ii 0.92 1.86 2.779 (3) 172
OW4—H941···O10i 0.93 1.86 2.761 (4) 163

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RU2003).

References

  1. Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst. 32, 115–119.
  2. Brandenburg, K. & Berndt, M. (2001). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. Duisenberg, A. J. M. (1992). J. Appl. Cryst. 25, 92–96.
  4. Duisenberg, A. J. M., Kroon-Batenburg, L. M. J. & Schreurs, A. M. M. (2003). J. Appl. Cryst. 36, 220–229.
  5. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  6. Kazerouni, M. R., Hedberg, L. & Hedberg, K. (1994). J. Am. Chem. Soc. 116, 5279–5284.
  7. Mahé, N. & Bataille, T. (2004). Inorg. Chem. 43, 8379–8386. [DOI] [PubMed]
  8. Mathew, S., Paul, G., Shivasankar, K., Choudhury, A. & Rao, C. N. R. (2002). J. Mol. Struct. 641, 263–279.
  9. Meulenaer, J. de & Tompa, H. (1965). Acta Cryst. 19, 1014–1018.
  10. Nonius (2000). COLLECT, Nonius BV, Delft, The Netherlands.
  11. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  12. Zenkhri, L., Bataille, T. & Audebrand, N. (2011). Acta Cryst. E67, o1118. [DOI] [PMC free article] [PubMed]

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811011251/ru2003sup1.cif

e-67-0m529-sup1.cif (30.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011251/ru2003Isup2.hkl

e-67-0m529-Isup2.hkl (240.7KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES