supplementary materials


Acta Cryst. (2009). E65, m842-m843    [ doi:10.1107/S1600536809023824 ]

Chlorido[(E)-2-hydroxy-6-(isonicotinoylhydrazonomethyl)phenyl]mercury(II) monohydrate

S.-Z. Bai, X.-H. Lou, H.-M. Li and H. Shi

Abstract top

The asymmetric unit of the title compound, [Hg(C13H10N3O2)Cl]·H2O, contains two independent mercury(II) complexes with slightly different conformations, related via a pseudo-inversion centre, and two water molecules. The HgII atoms show a typical linear geometry to a C atom of the benzene ring and to a Cl atom. A benzene C and the azomethine N atom chelate the HgII atoms with weak intramolecular Hg...N bonding distances of 2.735 (3) and 2.739 (3) Å, respectively. The resulting five-membered metallacycles are nearly coplanar with the benzene rings [dihedral angles = 0.9 (1) and 0.7 (1)°], while the pyridine rings make dihedral angles with the benzene units of 58.17 (1) and 56.58 (1)°. In the crystal structure, the HgII complexes are linked by hydroxy donor and pyridine acceptor groups into chains along [010]. The water molecules connect the complexes through intermolecular O-H...Ocarbonyl bonds in the a-axis direction, and the azomethine H atoms donate towards the water O atoms, forming a three-dimensional network of intermolecular O-H...N, O-H...O and N-H...O hydrogen bonds.

Comment top

Cyclometallated compounds have attracted much research interest owing to theirs utility in synthesis, catalysis and materials (Gruter et al., 1995; Xu et al., 2009b). Among them, cyclomercurated compounds are easy to prepare through a C—H activation process and are stable but reasonably reactive. Although numerous cyclomercurated compounds have been widely investigated, and many examples have been reported(Soro et al., 2005; Hao et al., 2007), only a few cyclometallated Schiff bases containing heterocyclic ring are known(Lin et al., 2002).

The asymmetric unit of the title compound (Fig.1) contains two independent mercury(II) complexes with slightly different conformations, related via a pseudo-inversion centre (1/2a, 3/4b, 1/4c), and two water molecules. The HgII atoms show a typical linear coordination geometry with a carbon atom of the benzene ring and the chloride atom in trans position. A benzene carbon and the azomethine nitrogen atom chelate the mercury(II) atoms with weak intramolecular Hg···N bonding distances of 2.735 (3)Å and 2.739 (3) Å. which are shorter than those of the related HgII complex (Hao et al., (2007); Lin et al., (2002); Xu et al., (2009a). The C—Hg and Hg—Cl bond distances are within normal ranges. The C1—Hg1—Cl1 and C14—Hg2—Cl2 angles are 173.85 (10)° and 174.67 (10)°, slightly smaller than the ideal value of 180° in organic derivatives of mercury. The resulting five-membered metallacycles are nearly coplanar with the benzene ring, while the pyridine are not coplanar with the benzene. In the crystal structure, intermolecular O—H···O, N—H···O and O—H···N hydrogen bonds (Table 1) link the independent HgII complexes and the water molecules into a three-dimensional network.

Related literature top

For general background, see: Gruter et al. (1995); Soro et al. (2005); Xu et al. (2009b). For related structures, see: Hao et al. (2007); Lin et al. (2002); For the synthesis, see: Xu et al. (2009a).

Experimental top

Chlorido(2-formyl-6-hydroxybenzaldehyde-kC1)mercury(II) was synthesized according to the reported procedure (Xu et al., 2009a). The title compound was prepared from the above compound with isonicotinoylhydrazine and recrystallized from ethanol solution at room temperature to give the desired product as colourless crystals suitable for single-crystal X-ray diffraction.

Refinement top

All H atoms were placed in geometrically idealized positions and constrained to ride on their patent atoms, with distances: C—H = 0.93 Å, N—H = 0.86 Å, and O—H = 0.82 Å. The Uiso(H) values were set at 1.2Ueq (C,N) and 1.5Ueq(O).

Computing details top

Data collection: SMART (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with displacement ellipsoids at the 30% probability level.
Chlorido[(E)-2-hydroxy-6-(isonicotinoylhydrazonomethyl)phenyl]mercury(II) monohydrate top
Crystal data top
[Hg(C13H10N3O2)Cl]·H2OF(000) = 1856
Mr = 494.30Dx = 2.160 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 14.5932 (16) ÅCell parameters from 5064 reflections
b = 14.0111 (15) Åθ = 2.7–28.3°
c = 15.3711 (17) ŵ = 10.31 mm1
β = 104.685 (1)°T = 296 K
V = 3040.2 (6) Å3Block, colorless
Z = 80.37 × 0.28 × 0.25 mm
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
5658 independent reflections
Radiation source: fine-focus sealed tube4683 reflections with I > 2σ(I)
graphiteRint = 0.030
φ and ω scansθmax = 25.5°, θmin = 2.2°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1717
Tmin = 0.113, Tmax = 0.179k = 1616
22798 measured reflectionsl = 1618
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)] = 0.021Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.046H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0197P)2 + 1.3364P]
where P = (Fo2 + 2Fc2)/3
5658 reflections(Δ/σ)max = 0.002
381 parametersΔρmax = 0.52 e Å3
0 restraintsΔρmin = 0.83 e Å3
Crystal data top
[Hg(C13H10N3O2)Cl]·H2OV = 3040.2 (6) Å3
Mr = 494.30Z = 8
Monoclinic, P21/nMo Kα radiation
a = 14.5932 (16) ŵ = 10.31 mm1
b = 14.0111 (15) ÅT = 296 K
c = 15.3711 (17) Å0.37 × 0.28 × 0.25 mm
β = 104.685 (1)°
Data collection top
Bruker SMART APEX CCD area-detector
diffractometer
5658 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
4683 reflections with I > 2σ(I)
Tmin = 0.113, Tmax = 0.179Rint = 0.030
22798 measured reflectionsθmax = 25.5°
Refinement top
R[F2 > 2σ(F2)] = 0.021H-atom parameters constrained
wR(F2) = 0.046Δρmax = 0.52 e Å3
S = 1.05Δρmin = 0.83 e Å3
5658 reflectionsAbsolute structure: ?
381 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
Hg10.909422 (9)0.795528 (10)0.140566 (10)0.03271 (5)
Hg20.088755 (10)0.667392 (10)0.363229 (10)0.03354 (5)
Cl11.06292 (6)0.74039 (8)0.15848 (7)0.0482 (3)
Cl20.06489 (7)0.72341 (8)0.34424 (7)0.0485 (3)
O10.85291 (17)1.00819 (18)0.13735 (19)0.0444 (7)
H10.84091.06410.12310.067*
O20.91602 (18)0.54581 (19)0.0795 (2)0.0539 (8)
O30.14451 (18)0.45504 (17)0.3573 (2)0.0473 (7)
H30.15650.39870.36930.071*
O40.08053 (18)0.91980 (18)0.4187 (2)0.0494 (7)
N10.7764 (2)0.6537 (2)0.1123 (2)0.0339 (7)
N20.7733 (2)0.55515 (19)0.11402 (19)0.0338 (7)
H2D0.72530.52550.12390.041*
N30.8374 (2)0.2013 (2)0.1131 (2)0.0397 (8)
N40.2225 (2)0.8089 (2)0.3911 (2)0.0362 (7)
N50.2266 (2)0.9077 (2)0.39086 (19)0.0352 (7)
H5D0.27600.93680.38360.042*
N60.1645 (2)1.2624 (2)0.3851 (2)0.0397 (8)
C10.7779 (2)0.8579 (2)0.1197 (2)0.0279 (8)
C20.7707 (3)0.9568 (3)0.1195 (2)0.0349 (8)
C30.6823 (3)1.0005 (3)0.1066 (3)0.0431 (10)
H3A0.67791.06670.10760.052*
C40.6011 (3)0.9454 (3)0.0924 (3)0.0495 (11)
H40.54220.97460.08300.059*
C50.6075 (3)0.8465 (3)0.0920 (3)0.0411 (9)
H50.55280.80970.08300.049*
C60.6953 (2)0.8023 (2)0.1051 (2)0.0313 (8)
C70.6986 (3)0.6972 (2)0.1046 (2)0.0331 (8)
H70.64300.66250.09860.040*
C80.8484 (3)0.5069 (2)0.0996 (2)0.0351 (9)
C90.8433 (2)0.4003 (2)0.1063 (2)0.0302 (8)
C100.8804 (2)0.3447 (2)0.0486 (3)0.0361 (9)
H100.90890.37310.00750.043*
C110.8744 (2)0.2467 (3)0.0532 (3)0.0379 (9)
H110.89730.21020.01270.046*
C120.8025 (3)0.2558 (3)0.1688 (3)0.0416 (9)
H120.77600.22540.21040.050*
C130.8035 (3)0.3542 (3)0.1680 (3)0.0393 (9)
H130.77820.38900.20790.047*
C140.2197 (2)0.6052 (2)0.3792 (2)0.0291 (8)
C150.3026 (3)0.6602 (2)0.3951 (2)0.0324 (8)
C160.3903 (3)0.6153 (3)0.4047 (3)0.0446 (10)
H160.44530.65180.41490.054*
C170.3955 (3)0.5171 (3)0.3992 (3)0.0510 (11)
H170.45400.48760.40570.061*
C180.3143 (3)0.4625 (3)0.3840 (3)0.0447 (10)
H180.31800.39650.37980.054*
C190.2271 (3)0.5063 (3)0.3751 (2)0.0350 (9)
C200.3007 (3)0.7648 (3)0.3986 (2)0.0361 (9)
H200.35680.79920.40630.043*
C210.1510 (2)0.9574 (3)0.4023 (2)0.0352 (8)
C220.1583 (2)1.0639 (2)0.3948 (2)0.0305 (8)
C230.1992 (3)1.1083 (3)0.3340 (2)0.0381 (9)
H230.22591.07270.29550.046*
C240.1997 (3)1.2072 (2)0.3315 (3)0.0392 (9)
H240.22651.23670.28960.047*
C250.1267 (3)1.2190 (3)0.4458 (3)0.0386 (9)
H250.10361.25670.48540.046*
C260.1205 (2)1.1212 (3)0.4521 (2)0.0372 (9)
H260.09191.09360.49350.045*
O50.89687 (19)0.9980 (2)0.33618 (19)0.0566 (8)
H1W0.94710.97520.36830.085*
H2W0.90021.00180.28290.085*
O60.10303 (19)0.4671 (2)0.1547 (2)0.0618 (8)
H3W0.08900.45810.20310.093*
H4W0.05710.48820.11610.093*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Hg10.03055 (8)0.02692 (10)0.04319 (9)0.00303 (6)0.01399 (6)0.00319 (6)
Hg20.03092 (8)0.02783 (10)0.04418 (9)0.00243 (6)0.01377 (6)0.00243 (6)
Cl10.0326 (5)0.0563 (7)0.0615 (7)0.0070 (4)0.0225 (5)0.0088 (5)
Cl20.0337 (5)0.0583 (7)0.0585 (7)0.0064 (4)0.0213 (5)0.0088 (5)
O10.0416 (15)0.0241 (15)0.0673 (19)0.0017 (11)0.0136 (14)0.0059 (13)
O20.0427 (16)0.0345 (16)0.092 (2)0.0030 (12)0.0304 (16)0.0051 (15)
O30.0496 (17)0.0181 (14)0.074 (2)0.0002 (12)0.0163 (14)0.0048 (14)
O40.0429 (16)0.0295 (16)0.081 (2)0.0021 (12)0.0254 (15)0.0056 (14)
N10.0407 (18)0.0175 (16)0.0423 (18)0.0007 (13)0.0085 (15)0.0004 (13)
N20.0329 (16)0.0204 (17)0.0505 (19)0.0019 (12)0.0151 (14)0.0009 (13)
N30.045 (2)0.026 (2)0.047 (2)0.0007 (13)0.0098 (16)0.0011 (14)
N40.0443 (19)0.0212 (17)0.0430 (19)0.0063 (14)0.0108 (15)0.0037 (14)
N50.0349 (17)0.0217 (17)0.0505 (19)0.0045 (13)0.0135 (14)0.0018 (14)
N60.0408 (18)0.0281 (19)0.050 (2)0.0005 (14)0.0120 (16)0.0004 (15)
C10.0333 (19)0.0218 (19)0.0300 (19)0.0068 (14)0.0103 (15)0.0038 (14)
C20.040 (2)0.028 (2)0.037 (2)0.0015 (16)0.0096 (17)0.0025 (16)
C30.048 (2)0.025 (2)0.057 (3)0.0112 (18)0.014 (2)0.0000 (18)
C40.042 (2)0.041 (3)0.063 (3)0.0197 (19)0.010 (2)0.004 (2)
C50.032 (2)0.035 (2)0.054 (3)0.0009 (16)0.0046 (18)0.0005 (18)
C60.036 (2)0.025 (2)0.034 (2)0.0047 (15)0.0097 (16)0.0003 (15)
C70.037 (2)0.025 (2)0.038 (2)0.0028 (15)0.0117 (17)0.0013 (16)
C80.036 (2)0.024 (2)0.044 (2)0.0021 (16)0.0075 (17)0.0039 (16)
C90.0301 (18)0.021 (2)0.037 (2)0.0014 (14)0.0052 (15)0.0032 (15)
C100.037 (2)0.029 (2)0.044 (2)0.0006 (16)0.0154 (18)0.0009 (17)
C110.039 (2)0.030 (2)0.046 (2)0.0082 (16)0.0132 (18)0.0025 (18)
C120.049 (2)0.037 (3)0.042 (2)0.0021 (18)0.0186 (19)0.0061 (19)
C130.052 (2)0.024 (2)0.044 (2)0.0024 (17)0.0164 (19)0.0021 (17)
C140.0347 (19)0.023 (2)0.0320 (19)0.0054 (14)0.0118 (16)0.0031 (15)
C150.038 (2)0.026 (2)0.033 (2)0.0030 (15)0.0092 (17)0.0014 (15)
C160.034 (2)0.040 (3)0.057 (3)0.0023 (17)0.0062 (19)0.0017 (19)
C170.038 (2)0.041 (3)0.070 (3)0.0165 (18)0.006 (2)0.005 (2)
C180.048 (2)0.026 (2)0.058 (3)0.0120 (18)0.009 (2)0.0042 (18)
C190.041 (2)0.023 (2)0.040 (2)0.0009 (16)0.0077 (17)0.0044 (16)
C200.034 (2)0.028 (2)0.046 (2)0.0025 (16)0.0108 (17)0.0024 (17)
C210.031 (2)0.032 (2)0.041 (2)0.0013 (16)0.0066 (17)0.0004 (17)
C220.0282 (18)0.023 (2)0.039 (2)0.0017 (14)0.0065 (16)0.0007 (16)
C230.047 (2)0.034 (2)0.037 (2)0.0030 (17)0.0175 (18)0.0026 (17)
C240.050 (2)0.026 (2)0.046 (2)0.0040 (16)0.0194 (19)0.0040 (17)
C250.040 (2)0.030 (2)0.048 (2)0.0069 (16)0.0135 (19)0.0033 (17)
C260.034 (2)0.040 (2)0.041 (2)0.0041 (16)0.0151 (17)0.0042 (17)
O50.0477 (17)0.068 (2)0.0577 (19)0.0121 (15)0.0196 (15)0.0016 (15)
O60.0449 (17)0.072 (2)0.071 (2)0.0108 (15)0.0201 (16)0.0060 (17)
Geometric parameters (Å, °) top
Hg1—C12.059 (3)C8—C91.501 (5)
Hg1—Cl12.3189 (9)C9—C131.390 (5)
Hg2—C142.058 (3)C9—C101.389 (5)
Hg2—Cl22.3231 (10)C10—C111.379 (5)
O1—C21.366 (4)C10—H100.9300
O1—H10.8200C11—H110.9300
O2—C81.233 (4)C12—C131.379 (5)
O3—C191.369 (4)C12—H120.9300
O3—H30.8200C13—H130.9300
O4—C211.237 (4)C14—C191.391 (5)
N1—C71.268 (4)C14—C151.402 (5)
N1—N21.382 (4)C15—C161.400 (5)
N2—C81.354 (4)C15—C201.468 (5)
N2—H2D0.8600C16—C171.383 (5)
N3—C121.340 (5)C16—H160.9300
N3—C111.341 (5)C17—C181.379 (5)
N4—C201.277 (4)C17—H170.9300
N4—N51.386 (4)C18—C191.389 (5)
N5—C211.353 (4)C18—H180.9300
N5—H5D0.8600C20—H200.9300
N6—C241.323 (4)C21—C221.502 (5)
N6—C251.345 (4)C22—C231.379 (5)
C1—C21.388 (5)C22—C261.402 (5)
C1—C61.405 (5)C23—C241.387 (5)
C2—C31.397 (5)C23—H230.9300
C3—C41.384 (5)C24—H240.9300
C3—H3A0.9300C25—C261.378 (5)
C4—C51.389 (5)C25—H250.9300
C4—H40.9300C26—H260.9300
C5—C61.392 (5)O5—H1W0.8363
C5—H50.9300O5—H2W0.8344
C6—C71.473 (5)O6—H3W0.8298
C7—H70.9300O6—H4W0.8293
C1—Hg1—Cl1173.85 (10)N3—C12—C13123.8 (3)
C14—Hg2—Cl2174.67 (10)N3—C12—H12118.1
C2—O1—H1109.5C13—C12—H12118.1
C19—O3—H3109.5C12—C13—C9118.5 (3)
C7—N1—N2116.7 (3)C12—C13—H13120.7
C8—N2—N1117.6 (3)C9—C13—H13120.7
C8—N2—H2D121.2C19—C14—C15118.8 (3)
N1—N2—H2D121.2C19—C14—Hg2119.7 (3)
C12—N3—C11117.0 (3)C15—C14—Hg2121.4 (2)
C20—N4—N5116.5 (3)C16—C15—C14119.8 (3)
C21—N5—N4118.5 (3)C16—C15—C20118.0 (3)
C21—N5—H5D120.7C14—C15—C20122.2 (3)
N4—N5—H5D120.7C17—C16—C15120.2 (4)
C24—N6—C25117.4 (3)C17—C16—H16119.9
C2—C1—C6119.5 (3)C15—C16—H16119.9
C2—C1—Hg1119.4 (3)C18—C17—C16120.2 (4)
C6—C1—Hg1121.1 (2)C18—C17—H17119.9
O1—C2—C1117.6 (3)C16—C17—H17119.9
O1—C2—C3122.0 (3)C17—C18—C19119.9 (4)
C1—C2—C3120.3 (3)C17—C18—H18120.0
C4—C3—C2120.0 (4)C19—C18—H18120.0
C4—C3—H3A120.0O3—C19—C18121.7 (3)
C2—C3—H3A120.0O3—C19—C14117.2 (3)
C3—C4—C5120.2 (3)C18—C19—C14121.0 (3)
C3—C4—H4119.9N4—C20—C15120.3 (3)
C5—C4—H4119.9N4—C20—H20119.9
C4—C5—C6120.2 (3)C15—C20—H20119.9
C4—C5—H5119.9O4—C21—N5123.6 (3)
C6—C5—H5119.9O4—C21—C22121.2 (3)
C5—C6—C1119.8 (3)N5—C21—C22115.2 (3)
C5—C6—C7118.3 (3)C23—C22—C26118.4 (3)
C1—C6—C7121.9 (3)C23—C22—C21123.4 (3)
N1—C7—C6120.6 (3)C26—C22—C21118.3 (3)
N1—C7—H7119.7C22—C23—C24118.3 (3)
C6—C7—H7119.7C22—C23—H23120.8
O2—C8—N2123.6 (3)C24—C23—H23120.8
O2—C8—C9121.0 (3)N6—C24—C23124.1 (3)
N2—C8—C9115.4 (3)N6—C24—H24117.9
C13—C9—C10118.2 (3)C23—C24—H24117.9
C13—C9—C8123.1 (3)N6—C25—C26122.9 (3)
C10—C9—C8118.7 (3)N6—C25—H25118.6
C11—C10—C9119.1 (3)C26—C25—H25118.6
C11—C10—H10120.5C25—C26—C22118.8 (3)
C9—C10—H10120.5C25—C26—H26120.6
N3—C11—C10123.3 (3)C22—C26—H26120.6
N3—C11—H11118.4H1W—O5—H2W110.1
C10—C11—H11118.4H3W—O6—H4W111.0
C7—N1—N2—C8163.9 (3)C8—C9—C13—C12179.9 (3)
C20—N4—N5—C21166.2 (3)Cl2—Hg2—C14—C192.9 (12)
Cl1—Hg1—C1—C223.9 (11)Cl2—Hg2—C14—C15176.6 (8)
Cl1—Hg1—C1—C6155.6 (7)C19—C14—C15—C161.2 (5)
C6—C1—C2—O1177.6 (3)Hg2—C14—C15—C16179.3 (3)
Hg1—C1—C2—O12.8 (4)C19—C14—C15—C20178.7 (3)
C6—C1—C2—C31.2 (5)Hg2—C14—C15—C201.8 (5)
Hg1—C1—C2—C3179.2 (3)C14—C15—C16—C170.4 (6)
O1—C2—C3—C4177.4 (4)C20—C15—C16—C17178.0 (4)
C1—C2—C3—C41.1 (6)C15—C16—C17—C180.1 (6)
C2—C3—C4—C50.8 (6)C16—C17—C18—C190.6 (6)
C3—C4—C5—C60.6 (6)C17—C18—C19—O3178.0 (4)
C4—C5—C6—C10.8 (6)C17—C18—C19—C141.4 (6)
C4—C5—C6—C7179.7 (3)C15—C14—C19—O3178.5 (3)
C2—C1—C6—C51.1 (5)Hg2—C14—C19—O32.1 (4)
Hg1—C1—C6—C5179.4 (3)C15—C14—C19—C181.7 (5)
C2—C1—C6—C7179.9 (3)Hg2—C14—C19—C18178.8 (3)
Hg1—C1—C6—C70.5 (5)N5—N4—C20—C15177.1 (3)
N2—N1—C7—C6178.0 (3)C16—C15—C20—N4179.3 (4)
C5—C6—C7—N1176.9 (3)C14—C15—C20—N43.2 (5)
C1—C6—C7—N14.2 (5)N4—N5—C21—O44.8 (5)
N1—N2—C8—O24.8 (5)N4—N5—C21—C22175.9 (3)
N1—N2—C8—C9177.4 (3)O4—C21—C22—C23143.1 (4)
O2—C8—C9—C13145.8 (4)N5—C21—C22—C2337.6 (5)
N2—C8—C9—C1336.3 (5)O4—C21—C22—C2636.2 (5)
O2—C8—C9—C1033.8 (5)N5—C21—C22—C26143.1 (3)
N2—C8—C9—C10144.1 (3)C26—C22—C23—C241.0 (5)
C13—C9—C10—C111.5 (5)C21—C22—C23—C24178.3 (3)
C8—C9—C10—C11178.9 (3)C25—N6—C24—C230.5 (6)
C12—N3—C11—C102.0 (5)C22—C23—C24—N61.1 (6)
C9—C10—C11—N32.5 (5)C24—N6—C25—C262.2 (5)
C11—N3—C12—C130.6 (5)N6—C25—C26—C222.3 (5)
N3—C12—C13—C90.2 (6)C23—C22—C26—C250.6 (5)
C10—C9—C13—C120.3 (5)C21—C22—C26—C25179.9 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O6—H4W···O2i0.832.152.898 (4)150
O6—H3W···O30.832.303.023 (4)146
O5—H2W···O10.832.172.963 (4)159
O5—H1W···O4ii0.842.062.876 (4)166
N5—H5D···O6iii0.862.042.872 (4)162
N2—H2D···O5iv0.862.062.890 (4)161
O3—H3···N6v0.821.922.737 (4)171
O1—H1···N3vi0.821.932.733 (4)167
Symmetry codes: (i) x−1, y, z; (ii) x+1, y, z; (iii) −x+1/2, y+1/2, −z+1/2; (iv) −x+3/2, y−1/2, −z+1/2; (v) x, y−1, z; (vi) x, y+1, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O6—H4W···O2i0.832.152.898 (4)150
O6—H3W···O30.832.303.023 (4)146
O5—H2W···O10.832.172.963 (4)159
O5—H1W···O4ii0.842.062.876 (4)166
N5—H5D···O6iii0.862.042.872 (4)162
N2—H2D···O5iv0.862.062.890 (4)161
O3—H3···N6v0.821.922.737 (4)171
O1—H1···N3vi0.821.932.733 (4)167
Symmetry codes: (i) x−1, y, z; (ii) x+1, y, z; (iii) −x+1/2, y+1/2, −z+1/2; (iv) −x+3/2, y−1/2, −z+1/2; (v) x, y−1, z; (vi) x, y+1, z.
Acknowledgements top

This work was supported by the High-Level Personnel to Start Research Fund of Pingdingshan University (No. 2006044).

references
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