supplementary materials


lh2394 scheme

Acta Cryst. (2007). E63, m1891    [ doi:10.1107/S1600536807023719 ]

Tetrakis(1,6-hexanediammonium) tetrakis(hydrogenarsenate) heptahydrate

M. J. Todd and W. T. A. Harrison

Abstract top

The title compound, 4C6H18N22+·4HAsO42-·7H2O, contains a complex network of organic cations, hydrogenarsenate anions and water molecules. One of the two distinct (HAsO4)2- anions shows the expected distinction between protonated and unprotonated As-O bond lengths. The component species interact by way of N-H...O and O-H...O hydrogen bonds, with the latter leading to distinct centrosymmetric (HAsO4)4 tetramers, in which the central linking O-H...O bond is assumed to be disordered about the inversion centre. Together, the cations and anions form an unusual three-dimensional framework encapsulating [100] channels occupied by the water molecules.

Comment top

The title compound, (I), was prepared as part of our ongoing studies of hydrogen bonding interactions in the molecular salts of arsenic oxo-anions (Wilkinson & Harrison, 2007a,b). Its asymmetric unit contains two organic cations, two anions and three-and-a-half water molecules (Fig. 1).

The tetrahedral (HAs1O4)2− anion in (I) shows the expected distinction (Table 1) between its protonated and unprotonated As—O bond lengths. The situation for the (HAs2O4)2− group is less clear cut, and seems to be correlated with disorder of its H atoms (see below). Both C2H10N22+ dications are in their extended conformations with all their backbone torsion angles close to 180°. Three fully occupied (O9, O10, O11) water molecules and one half occupied (O12) water molecule complete the structure. O12 cannot be more than half occupied due to a close O12···O12xx (xx = −x, 1 − y, −z) contact of 2.21 (1) Å.

As well as Coulombic forces, the component species in (I) interact by way of a network of N—H···O and O—H···O hydrogen bonds (Table 2). The (HAsO4)2− units are linked by way of O—H···O bonds into distinctive, isolated, tetramers (Fig. 2). The complete assembly is generated by inversion, thus the central O5—H2···O5i (see Table 2 for symmetry code) link must be disordered (i.e. O5—H2···O5i + O5i—H2i···O5 bonds) or possibly a symmetric O5···H2···O5i bond (i.e. the H atom occupies the inversion centre (Wilson, 2001). These possibilities could not be distinguished in the present experiment and a disordered model was assumed. Either of these possibilities necessitates disorder of the H atoms of the As2-hydrogenarsenate group, with one of the (HAsO4)2− moieties directing its H atom elsewhere. The extended As2—O6 bond length suggests that O6 bears the H atom and if so, it makes an O—H···O link to the disordered O12 water molecule O atom (Fig. 2).

The cations interact with the anion tetramers by way of a large number of N—H···O bonds (Table 2), with each NH3+ group making three such links, as is typically seen in these systems (Wilkinson & Harrison, 2007a). Unfortunately the H atoms of the water molecules in (I) could not be located in the present study. The disorder of the As2 H atoms and O12 seems to require that at least some of the water H atoms are also disordered, and the situation is too uncertain to allow their geometrical placement with any confidence.

The packing for (I) results in a distinctive structure (Fig. 3) in which hydrogen-bonded (001) sheets of tetrahedral tetramers are bridged by the organic molecules to result in a framework encapsulating [100] channels, which are occupied by the water molecules.

The structure of 1,6-diamminiumhexane bis(dihydrogenarsenate), C6H18N2·(H2AsO4)2, (II), (Wilkinson & Harrison, 2007a), in which the arsenic-containing anion bears two protons, is entirely different to that of (I). In (II), infinite sheets of H-bonded tetrahedra arise and the centrosymmetric cation adopts a gauche conformation. Other types of supramolecular networks based on hydrogen bonded organic cations and arsenate tetrahedra are descibed by Wilkinson & Harrison (2007b).

Related literature top

For related structures and background literature, see: Wilkinson & Harrison (2007a,b); Wilson (2001).

Experimental top

0.5 M Aqueous solutions of 1,6-diaminohexane (10 ml) and arsenic acid (10 ml) were mixed, resulting in a colourless liquid. Aqueous ammonia was then added to the mixture to raise the pH to 11. Colourless slabs of (I) grew as the water slowly evaporated at 298 K.

Refinement top

The highest difference peak is 0.82Å from As2, and the deepest difference hole is 0.62Å from As2 perhaps indicating disorder of the (HAs2O4)2− group, but refinements attempting to model this were unstable. The next-highest feature in the final difference map (0.76 e Å3) is at the noise level.

H1 was located in a difference map and refined as riding. H2, H3 and the C– and N-bonded hydrogen atoms were placed in idealized positions (O—H = 0.90 Å, C—H = 0.99 Å, N—H = 0.91 Å) and refined as riding with Uiso(H) = 1.2Ueq(carrier).

The H atoms of the water molecules could not be located.

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: HKL SCALEPACK (Otwinowski & Minor, 1997); data reduction: HKL DENZO and SCALEPACK (Otwinowski & Minor, 1997) and SORTAV (Blessing, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) (50% displacement ellipsoids; H atoms are drawn as spheres of arbitrary radius).
[Figure 2] Fig. 2. A tetramer of (HAsO4)2− tetrahedra in (I) with with the H bonds indicated by double-dashed lines. Symmetry code as in Table 2. Only one disorder component for H2, H3 and O12 is shown.
[Figure 3] Fig. 3. Unit cell packing in (I) showing the (001) hydrogenarsenate layers bridged by the organic cations, with H bonds indicated by pale blue lines. The water O atoms (pink spheres) occupy [100] channels.
tetra(1,6-hexanediammonium) tetra(hydrogenarsenate) heptahydrate top
Crystal data top
4C6H18N22+·4HAsO42–·7H2OZ = 1
Mr = 1158.72F000 = 606
Triclinic, P1Dx = 1.521 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 10.2206 (2) ÅCell parameters from 5718 reflections
b = 11.2773 (4) Åθ = 2.9–27.5º
c = 12.7211 (4) ŵ = 2.70 mm1
α = 109.6648 (12)ºT = 120 (2) K
β = 108.0176 (18)ºSlab, colourless
γ = 97.7941 (18)º0.42 × 0.22 × 0.06 mm
V = 1265.11 (6) Å3
Data collection top
Bruker-Nonius KappaCCD
diffractometer
5804 independent reflections
Radiation source: fine-focus sealed tube4788 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.053
T = 120(2) Kθmax = 27.6º
ω and φ scansθmin = 3.3º
Absorption correction: multi-scan
(SADABS; Bruker, 2003)
h = 13→13
Tmin = 0.397, Tmax = 0.855k = 14→14
25594 measured reflectionsl = 16→16
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difmap and geom
R[F2 > 2σ(F2)] = 0.047H-atom parameters constrained
wR(F2) = 0.126  w = 1/[σ2(Fo2) + (0.0593P)2 + 3.4341P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
5804 reflectionsΔρmax = 3.79 e Å3
275 parametersΔρmin = 1.87 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
4C6H18N22+·4HAsO42–·7H2Oγ = 97.7941 (18)º
Mr = 1158.72V = 1265.11 (6) Å3
Triclinic, P1Z = 1
a = 10.2206 (2) ÅMo Kα
b = 11.2773 (4) ŵ = 2.70 mm1
c = 12.7211 (4) ÅT = 120 (2) K
α = 109.6648 (12)º0.42 × 0.22 × 0.06 mm
β = 108.0176 (18)º
Data collection top
Bruker-Nonius KappaCCD
diffractometer
5804 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2003)
4788 reflections with I > 2σ(I)
Tmin = 0.397, Tmax = 0.855Rint = 0.053
25594 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.047275 parameters
wR(F2) = 0.126H-atom parameters constrained
S = 1.07Δρmax = 3.79 e Å3
5804 reflectionsΔρmin = 1.87 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 > 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*/UeqOcc. (<1)
As10.26080 (3)0.19642 (3)0.50711 (3)0.01311 (11)
O10.3494 (3)0.3195 (3)0.6417 (2)0.0214 (6)
O20.3187 (3)0.0621 (2)0.4901 (2)0.0183 (5)
O30.0842 (3)0.1579 (3)0.4714 (2)0.0204 (5)
O40.2927 (3)0.2388 (3)0.3965 (2)0.0208 (6)
H10.28580.32030.41260.025*
As20.21274 (4)0.58973 (4)0.44105 (4)0.02178 (12)
O50.0387 (3)0.5234 (3)0.4168 (3)0.0289 (6)
H20.01250.50750.47320.035*0.50
O60.1964 (3)0.6605 (3)0.3415 (3)0.0309 (7)
H30.14600.60940.26320.037*0.50
O70.2942 (3)0.7031 (2)0.5818 (2)0.0206 (5)
O80.2976 (3)0.4749 (2)0.4154 (2)0.0219 (6)
N10.4702 (3)0.0659 (3)0.6085 (3)0.0160 (6)
H1A0.53630.08100.57500.019*
H1B0.41550.02100.57470.019*
H1C0.41370.14340.59490.019*
C10.5434 (4)0.0118 (4)0.7400 (3)0.0170 (7)
H1D0.61660.08910.75490.020*
H1E0.59250.04170.77820.020*
C20.4383 (4)0.0566 (4)0.7969 (3)0.0185 (7)
H2A0.36620.02060.78360.022*
H2B0.38790.10880.75770.022*
C30.5151 (4)0.1388 (4)0.9319 (3)0.0194 (7)
H3A0.59180.21200.94440.023*
H3B0.56080.08430.97070.023*
C40.4182 (4)0.1948 (4)0.9946 (3)0.0203 (8)
H4A0.36910.24690.95450.024*
H4B0.34430.12220.98670.024*
C50.5023 (4)0.2805 (4)1.1273 (3)0.0186 (7)
H5A0.57840.35091.13480.022*
H5B0.54880.22731.16740.022*
C60.4099 (4)0.3416 (4)1.1915 (3)0.0174 (7)
H6A0.35970.39181.14970.021*
H6B0.33710.27171.18860.021*
N20.4985 (3)0.4299 (3)1.3197 (3)0.0164 (6)
H2C0.44050.45391.36010.020*
H2D0.55340.50241.32250.020*
H2E0.55580.38751.35460.020*
N30.0774 (3)0.2552 (3)0.6731 (3)0.0237 (7)
H3C0.15280.25350.64940.028*
H3D0.02060.20990.64210.028*
H3E0.02620.33950.64580.028*
C70.1305 (4)0.1947 (5)0.8063 (4)0.0283 (9)
H7A0.17860.10110.83480.034*
H7B0.20240.23680.83950.034*
C80.0135 (4)0.2063 (4)0.8551 (4)0.0236 (8)
H8A0.04520.29800.81760.028*
H8B0.04950.15110.83530.028*
C90.0814 (4)0.1622 (4)0.9913 (3)0.0239 (8)
H9A0.14580.21711.00900.029*
H9B0.14090.07101.02660.029*
C100.0225 (4)0.1685 (4)1.0540 (3)0.0225 (8)
H10A0.07750.10361.04830.027*
H10B0.09070.25641.01330.027*
C110.0575 (4)0.1407 (4)1.1859 (3)0.0204 (8)
H11A0.11770.20201.19020.025*
H11B0.12200.05111.22620.025*
C120.0375 (4)0.1525 (4)1.2549 (3)0.0200 (7)
H12A0.08480.08081.26480.024*
H12B0.11250.23661.20910.024*
N40.0499 (3)0.1459 (3)1.3753 (3)0.0177 (6)
H4C0.00650.14891.41800.021*
H4D0.12090.07001.41590.021*
H4E0.08880.21491.36580.021*
O90.8047 (3)0.5471 (3)1.2428 (3)0.0365 (7)
O100.6206 (4)0.3245 (3)0.7704 (4)0.0487 (10)
O110.7583 (5)0.5024 (5)1.0047 (4)0.0727 (14)
O120.0334 (8)0.4948 (8)0.0893 (7)0.0505 (19)0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
As10.01328 (18)0.01261 (18)0.01532 (19)0.00403 (13)0.00671 (14)0.00644 (14)
O10.0217 (13)0.0167 (13)0.0159 (13)0.0013 (10)0.0032 (10)0.0001 (10)
O20.0250 (13)0.0156 (12)0.0212 (13)0.0100 (10)0.0114 (11)0.0112 (11)
O30.0103 (11)0.0293 (14)0.0210 (14)0.0025 (10)0.0065 (10)0.0099 (12)
O40.0324 (15)0.0173 (13)0.0246 (14)0.0104 (11)0.0193 (12)0.0134 (11)
As20.0211 (2)0.0165 (2)0.0222 (2)0.00862 (15)0.00423 (16)0.00361 (16)
O50.0213 (14)0.0269 (15)0.0310 (16)0.0043 (12)0.0083 (12)0.0051 (13)
O60.0370 (17)0.0348 (17)0.0321 (17)0.0191 (13)0.0139 (13)0.0221 (14)
O70.0204 (13)0.0176 (13)0.0183 (13)0.0024 (10)0.0059 (11)0.0031 (11)
O80.0278 (14)0.0156 (12)0.0282 (15)0.0102 (11)0.0147 (12)0.0103 (11)
N10.0163 (14)0.0159 (14)0.0191 (16)0.0055 (11)0.0085 (12)0.0087 (12)
C10.0150 (16)0.0198 (17)0.0175 (18)0.0056 (14)0.0073 (14)0.0076 (15)
C20.0154 (16)0.0204 (18)0.0162 (18)0.0033 (14)0.0065 (14)0.0031 (15)
C30.0173 (17)0.0229 (18)0.0160 (18)0.0061 (14)0.0068 (14)0.0050 (15)
C40.0144 (17)0.0219 (18)0.0178 (18)0.0029 (14)0.0042 (14)0.0022 (15)
C50.0154 (17)0.0233 (18)0.0154 (18)0.0042 (14)0.0066 (14)0.0054 (15)
C60.0135 (16)0.0193 (17)0.0154 (17)0.0019 (13)0.0041 (13)0.0044 (14)
N20.0174 (14)0.0169 (14)0.0149 (15)0.0053 (12)0.0061 (12)0.0061 (12)
N30.0174 (15)0.0352 (19)0.0227 (17)0.0067 (14)0.0088 (13)0.0155 (15)
C70.0175 (18)0.048 (3)0.022 (2)0.0078 (17)0.0079 (16)0.0177 (19)
C80.0168 (18)0.036 (2)0.022 (2)0.0053 (16)0.0078 (15)0.0164 (18)
C90.0164 (18)0.036 (2)0.021 (2)0.0052 (16)0.0066 (15)0.0158 (18)
C100.0153 (17)0.031 (2)0.0212 (19)0.0030 (15)0.0062 (15)0.0127 (17)
C110.0160 (17)0.028 (2)0.0203 (19)0.0048 (15)0.0079 (14)0.0127 (16)
C120.0170 (17)0.0246 (19)0.0168 (18)0.0036 (14)0.0045 (14)0.0088 (15)
N40.0191 (15)0.0153 (14)0.0185 (16)0.0018 (12)0.0076 (12)0.0072 (12)
O90.0394 (18)0.0360 (18)0.0305 (17)0.0069 (14)0.0184 (14)0.0056 (14)
O100.0305 (18)0.0350 (19)0.064 (3)0.0062 (14)0.0029 (16)0.0200 (18)
O110.062 (3)0.105 (4)0.048 (3)0.011 (3)0.015 (2)0.036 (3)
O120.040 (4)0.054 (5)0.040 (4)0.002 (3)0.006 (3)0.010 (4)
Geometric parameters (Å, °) top
As1—O11.667 (3)C6—H6A0.9900
As1—O21.671 (2)C6—H6B0.9900
As1—O31.674 (2)N2—H2C0.9100
As1—O41.734 (2)N2—H2D0.9100
O4—H10.8895N2—H2E0.9100
As2—O81.652 (3)N3—C71.478 (5)
As2—O71.668 (3)N3—H3C0.9100
As2—O61.689 (3)N3—H3D0.9100
As2—O51.721 (3)N3—H3E0.9100
O5—H20.8999C7—C81.518 (5)
O6—H30.8975C7—H7A0.9900
N1—C11.479 (5)C7—H7B0.9900
N1—H1A0.9100C8—C91.521 (5)
N1—H1B0.9100C8—H8A0.9900
N1—H1C0.9100C8—H8B0.9900
C1—C21.522 (5)C9—C101.519 (5)
C1—H1D0.9900C9—H9A0.9900
C1—H1E0.9900C9—H9B0.9900
C2—C31.524 (5)C10—C111.519 (5)
C2—H2A0.9900C10—H10A0.9900
C2—H2B0.9900C10—H10B0.9900
C3—C41.528 (5)C11—C121.517 (5)
C3—H3A0.9900C11—H11A0.9900
C3—H3B0.9900C11—H11B0.9900
C4—C51.517 (5)C12—N41.486 (5)
C4—H4A0.9900C12—H12A0.9900
C4—H4B0.9900C12—H12B0.9900
C5—C61.519 (5)N4—H4C0.9100
C5—H5A0.9900N4—H4D0.9100
C5—H5B0.9900N4—H4E0.9100
C6—N21.489 (4)
O1—As1—O2114.20 (13)H6A—C6—H6B108.1
O1—As1—O3112.72 (13)C6—N2—H2C109.5
O2—As1—O3109.82 (13)C6—N2—H2D109.5
O1—As1—O4109.54 (13)H2C—N2—H2D109.5
O2—As1—O4101.96 (12)C6—N2—H2E109.5
O3—As1—O4107.90 (13)H2C—N2—H2E109.5
As1—O4—H1106.7H2D—N2—H2E109.5
O8—As2—O7111.21 (13)C7—N3—H3C109.5
O8—As2—O6111.64 (14)C7—N3—H3D109.5
O7—As2—O6110.05 (14)H3C—N3—H3D109.5
O8—As2—O5110.83 (14)C7—N3—H3E109.5
O7—As2—O5109.28 (13)H3C—N3—H3E109.5
O6—As2—O5103.56 (15)H3D—N3—H3E109.5
As2—O5—H2123.3N3—C7—C8113.4 (3)
As2—O6—H3117.5N3—C7—H7A108.9
C1—N1—H1A109.5C8—C7—H7A108.9
C1—N1—H1B109.5N3—C7—H7B108.9
H1A—N1—H1B109.5C8—C7—H7B108.9
C1—N1—H1C109.5H7A—C7—H7B107.7
H1A—N1—H1C109.5C7—C8—C9109.0 (3)
H1B—N1—H1C109.5C7—C8—H8A109.9
N1—C1—C2111.2 (3)C9—C8—H8A109.9
N1—C1—H1D109.4C7—C8—H8B109.9
C2—C1—H1D109.4C9—C8—H8B109.9
N1—C1—H1E109.4H8A—C8—H8B108.3
C2—C1—H1E109.4C10—C9—C8115.5 (3)
H1D—C1—H1E108.0C10—C9—H9A108.4
C1—C2—C3110.9 (3)C8—C9—H9A108.4
C1—C2—H2A109.5C10—C9—H9B108.4
C3—C2—H2A109.5C8—C9—H9B108.4
C1—C2—H2B109.5H9A—C9—H9B107.5
C3—C2—H2B109.5C11—C10—C9110.4 (3)
H2A—C2—H2B108.0C11—C10—H10A109.6
C2—C3—C4114.2 (3)C9—C10—H10A109.6
C2—C3—H3A108.7C11—C10—H10B109.6
C4—C3—H3A108.7C9—C10—H10B109.6
C2—C3—H3B108.7H10A—C10—H10B108.1
C4—C3—H3B108.7C12—C11—C10114.5 (3)
H3A—C3—H3B107.6C12—C11—H11A108.6
C5—C4—C3111.5 (3)C10—C11—H11A108.6
C5—C4—H4A109.3C12—C11—H11B108.6
C3—C4—H4A109.3C10—C11—H11B108.6
C5—C4—H4B109.3H11A—C11—H11B107.6
C3—C4—H4B109.3N4—C12—C11109.6 (3)
H4A—C4—H4B108.0N4—C12—H12A109.7
C4—C5—C6112.9 (3)C11—C12—H12A109.7
C4—C5—H5A109.0N4—C12—H12B109.7
C6—C5—H5A109.0C11—C12—H12B109.7
C4—C5—H5B109.0H12A—C12—H12B108.2
C6—C5—H5B109.0C12—N4—H4C109.5
H5A—C5—H5B107.8C12—N4—H4D109.5
N2—C6—C5110.7 (3)H4C—N4—H4D109.5
N2—C6—H6A109.5C12—N4—H4E109.5
C5—C6—H6A109.5H4C—N4—H4E109.5
N2—C6—H6B109.5H4D—N4—H4E109.5
C5—C6—H6B109.5
N1—C1—C2—C3178.9 (3)N3—C7—C8—C9170.5 (4)
C1—C2—C3—C4176.4 (3)C7—C8—C9—C10179.8 (4)
C2—C3—C4—C5177.4 (3)C8—C9—C10—C11172.1 (3)
C3—C4—C5—C6178.1 (3)C9—C10—C11—C12176.6 (3)
C4—C5—C6—N2177.1 (3)C10—C11—C12—N4170.3 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O4—H1···O80.891.722.584 (4)163
O5—H2···O5i0.901.762.657 (6)180
O6—H3···O120.902.002.894 (8)180
N1—H1A···O2ii0.911.932.814 (4)164
N1—H1B···O20.911.812.717 (4)171
N1—H1C···O7iii0.911.902.810 (4)174
N2—H2C···O8iv0.911.822.716 (4)169
N2—H2D···O1v0.911.952.836 (4)165
N2—H2E···O7v0.912.062.965 (4)171
N3—H3C···O7iii0.911.942.826 (4)166
N3—H3D···O3vi0.911.832.699 (4)158
N3—H3E···O5vi0.911.892.779 (5)166
N4—H4C···O3vii0.911.842.735 (4)167
N4—H4D···O2iv0.912.062.941 (4)162
N4—H4E···O6viii0.911.902.801 (4)169
Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x+1, −y, −z+1; (iii) x, y−1, z; (iv) x, y, z+1; (v) −x+1, −y+1, −z+2; (vi) −x, −y, −z+1; (vii) −x, −y, −z+2; (viii) x, y−1, z+1.
Selected geometric parameters (Å) top
As1—O11.667 (3)As2—O81.652 (3)
As1—O21.671 (2)As2—O71.668 (3)
As1—O31.674 (2)As2—O61.689 (3)
As1—O41.734 (2)As2—O51.721 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O4—H1···O80.891.722.584 (4)163
O5—H2···O5i0.901.762.657 (6)180
O6—H3···O120.902.002.894 (8)180
N1—H1A···O2ii0.911.932.814 (4)164
N1—H1B···O20.911.812.717 (4)171
N1—H1C···O7iii0.911.902.810 (4)174
N2—H2C···O8iv0.911.822.716 (4)169
N2—H2D···O1v0.911.952.836 (4)165
N2—H2E···O7v0.912.062.965 (4)171
N3—H3C···O7iii0.911.942.826 (4)166
N3—H3D···O3vi0.911.832.699 (4)158
N3—H3E···O5vi0.911.892.779 (5)166
N4—H4C···O3vii0.911.842.735 (4)167
N4—H4D···O2iv0.912.062.941 (4)162
N4—H4E···O6viii0.911.902.801 (4)169
Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x+1, −y, −z+1; (iii) x, y−1, z; (iv) x, y, z+1; (v) −x+1, −y+1, −z+2; (vi) −x, −y, −z+1; (vii) −x, −y, −z+2; (viii) x, y−1, z+1.
Acknowledgements top

We thank the EPSRC National Crystallography Service (University of Southampton) for the data collection.

references
References top

Blessing, R. H. (1995). Acta Cryst. A51, 33–38.

Bruker (2003). SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565–?.

Nonius (1998). COLLECT. Nonius BV, Delft, The Netherlands.

Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.

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

Wilkinson, H. S. & Harrison, W. T. A. (2007a). Acta Cryst. E63, m902–m904.

Wilkinson, H. S. & Harrison, W. T. A. (2007b). Acta Cryst. E63, m1610–m1612.

Wilson, C. C. (2001). Acta Cryst. B57, 435–439.