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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 11;67(Pt 1):m59. doi: 10.1107/S1600536810051184

(meso-5,5,7,12,12,14-Hexamethyl-1,4,8,11-tetra­aza­cyclo­tetra­deca­ne)nickel(II) bis­[O,O′-bis­(4-methyl­phen­yl) thio­phosphate]

Yang-Guang Xiang a, Bin Xie b,*, Li-Ke Zou b, Jian-Shen Feng a, Chuan Lai a
PMCID: PMC3050336  PMID: 21522577

Abstract

In the centrosymmetric title complex, [Ni(C16H36N4)](C14H14O3PS)2, the NiII ion is coordinated by four N atoms and two O atoms within a slightly distorted NiN4O2 octa­hedral geometry. The asymmetric unit consits of one NiII ion that is located on a center of inversion, half of the macrocylic ligand and one anion occupying general positions. Intra­molecular N—H⋯O and N—H⋯S hydrogen bonding is found between the macrocyclic ligand and the monothio­phosphate anion.

Related literature

For the synthesis of O,O′-bis­(4-methyl­phen­yl) monothio­phos­phate, see: Pesin & Khaletakii (1961 ▶). For related structures, see: Feng et al. (2010 ▶); He et al. (2010 ▶); Zou et al. (2010 ▶).graphic file with name e-67-00m59-scheme1.jpg

Experimental

Crystal data

  • [Ni(C16H36N4)](C14H14O3PS)2

  • M r = 929.76

  • Monoclinic, Inline graphic

  • a = 10.977 (2) Å

  • b = 16.360 (3) Å

  • c = 12.767 (3) Å

  • β = 94.85 (3)°

  • V = 2284.6 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.64 mm−1

  • T = 113 K

  • 0.24 × 0.23 × 0.22 mm

Data collection

  • Rigaku Saturn CCD area-detector diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.862, T max = 0.873

  • 18654 measured reflections

  • 5376 independent reflections

  • 2665 reflections with I > 2σ(I)

  • R int = 0.101

Refinement

  • R[F 2 > 2σ(F 2)] = 0.053

  • wR(F 2) = 0.122

  • S = 0.99

  • 5376 reflections

  • 281 parameters

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

  • Δρmax = 0.97 e Å−3

  • Δρmin = −0.91 e Å−3

Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810051184/nc2207sup1.cif

e-67-00m59-sup1.cif (25.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810051184/nc2207Isup2.hkl

e-67-00m59-Isup2.hkl (263.3KB, 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—H1⋯S1i 0.92 (3) 2.66 (3) 3.574 (3) 171 (3)
N2—H2⋯O2 0.96 (3) 2.27 (3) 3.234 (3) 178 (3)

Symmetry code: (i) Inline graphic.

Acknowledgments

This work was supported by the Education Committee (No. 09ZA057) and the Science and Technology Committee (No. 2010GZ0130) of Sichuan Province, the Science and Technology Office of Zigong City (Nos. 08X01 and 10X05) and the Graduate Student Innovation Fund of Sichuan University of Science & Engineering (No. Y2009023).

supplementary crystallographic information

Comment

In our research on tetramine macrocycles transition metal complexes as mimetic hydrolases, we have recently reported several structures of their adducts with O,O'-dialkyldithiophosphate (He et al., 2010; Feng et al., 2010; Zou et al., 2010). Herein, we report the structure of an analogous O,O'-dialkylmonothiophosphate adducts, [Ni(meso-hmta)][OP(S)(OC6H4Me-4)2]2, where meso-hmta is meso-5,5,7,12,12,14-Hexamethyl-1,4,8,11-tetraazacyclotetradecane and (4-MeC6H4O)2(S)PO- is O,O'-bis(4-methylphenyl) monothiophosphate.

In the crystal structure of the title complex, the NiII ion is located on a center of inversion and possesses a slightly distorted NiN4O2 octahedral geometry (Fig. 1). The tetraamine macrocycle meso-hmta folds around the NiII centre at equatorial position and two O atoms from symmetry related O,O'-bis(4-methylphenyl) monothiophosphates are located in axial positions (Fig. 1). Intramolecular N—H···O and N—H···S hydrogen bonds are present between meso-hmta and monothiophosphates ligands (table 1). Furthermore, there exists a pair of symmetry related weak intermolecular C—H···π interactions for (C14—H14C)···C3(phenyl) between each couple of adjacent monothiophosphate ligands, which link the molecules into one-dimensional chains along [010]. The P1—O3 and P1—S1 bond lengths are 1.491 (2) and 1.9372 (14) Å respectively, corresponding to a delocalization of the negative charge over the O3—P1—S1 fragment.

Experimental

The ammonium O,O'-bis(4-methylphenyl)monothiophosphate was prepared according to the procedure described by Pesin (1961).

A solution of meso-5,5,7,12,12,14- hexamethyl-1,4,8,11- tetraazacyclotetradecane dihydrate (0.64 g, 2 mmol) and Ni(OAc)2.4H2O (0.50 g, 2 mmol) in 20 mL methanol was added to a solution of ammonium O,O'-bis(4-methylphenyl)monothiophosphate (4 mmol, 1.24 g) in 60 mL methanol. The mixture was refluxed for 6 h at 353 K and then filtered after cooling to room temperature. The filtrate was kept at room temperature and orange block crystals were obtained after 4 weeks.

Refinement

H atoms attached to C atoms were fixed geometrically and treated as riding, with C—H = 1.00Å (methine), 0.99Å (methylene), 0.98Å (methyl), 0.95Å (aromatic). The Uiso(H) = 1.5Ueq(C) for methyl groups and Uiso(H) = 1.2Ueq(C) for all other carbon bound H atoms. H atoms on N atoms were located in the difference map and refined isotropically.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title complex, showing the atom-numbering scheme with displacement ellipsoids drawn at 30% probability level. H atoms on N are represented as small spheres of arbitary radii and H atoms on C have been omitted for the sake of clarity. Hydrogen-bonds are shown as dashed lines. [Symmetry code: (i) -x + 1, -y + 1, -z + 1].

Crystal data

[Ni(C16H36N4)](C14H14O3PS)2 F(000) = 988
Mr = 929.76 Dx = 1.352 Mg m−3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 7232 reflections
a = 10.977 (2) Å θ = 2.2–27.9°
b = 16.360 (3) Å µ = 0.64 mm−1
c = 12.767 (3) Å T = 113 K
β = 94.85 (3)° Block, orange
V = 2284.6 (8) Å3 0.24 × 0.23 × 0.22 mm
Z = 2

Data collection

Rigaku Saturn CCD area-detector diffractometer 5376 independent reflections
Radiation source: rotating anode 2665 reflections with I > 2σ(I)
confocal Rint = 0.101
Detector resolution: 7.31 pixels mm-1 θmax = 27.9°, θmin = 2.2°
φ and ω scans h = −14→13
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −21→19
Tmin = 0.862, Tmax = 0.873 l = −16→16
18654 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)] = 0.053 Hydrogen site location: mixed
wR(F2) = 0.122 H atoms treated by a mixture of independent and constrained refinement
S = 0.99 w = 1/[σ2(Fo2) + (0.0244P)2] where P = (Fo2 + 2Fc2)/3
5376 reflections (Δ/σ)max < 0.001
281 parameters Δρmax = 0.97 e Å−3
0 restraints Δρmin = −0.91 e Å−3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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)

x y z Uiso*/Ueq
Ni1 0.5000 0.5000 0.5000 0.02073 (17)
P1 0.49238 (7) 0.69655 (5) 0.59137 (7) 0.0216 (2)
S1 0.57082 (7) 0.69510 (5) 0.73310 (7) 0.0288 (2)
O1 0.38094 (17) 0.76174 (13) 0.58832 (18) 0.0236 (6)
O2 0.58179 (16) 0.73444 (12) 0.50834 (17) 0.0214 (5)
O3 0.44815 (16) 0.61948 (12) 0.53863 (17) 0.0223 (5)
N1 0.3899 (2) 0.50845 (17) 0.3600 (2) 0.0219 (6)
H1 0.395 (3) 0.4578 (19) 0.329 (3) 0.035 (10)*
N2 0.6334 (2) 0.55494 (16) 0.4156 (2) 0.0215 (7)
H2 0.616 (3) 0.6087 (18) 0.441 (3) 0.030 (9)*
C1 0.2889 (3) 0.76449 (19) 0.5047 (3) 0.0223 (8)
C2 0.3144 (3) 0.76956 (19) 0.4017 (3) 0.0246 (8)
H2A 0.3966 0.7682 0.3837 0.030*
C3 0.2189 (3) 0.7767 (2) 0.3242 (3) 0.0275 (8)
H3 0.2366 0.7805 0.2528 0.033*
C4 0.0970 (3) 0.77851 (19) 0.3485 (3) 0.0250 (8)
C5 0.0746 (3) 0.7723 (2) 0.4531 (3) 0.0278 (9)
H5 −0.0073 0.7727 0.4719 0.033*
C6 0.1699 (3) 0.7656 (2) 0.5310 (3) 0.0296 (9)
H6 0.1531 0.7617 0.6026 0.035*
C7 −0.0083 (3) 0.7901 (2) 0.2647 (3) 0.0389 (10)
H7A −0.0184 0.7405 0.2218 0.058*
H7C 0.0093 0.8365 0.2198 0.058*
H7B −0.0837 0.8009 0.2984 0.058*
C8 0.6458 (3) 0.80740 (19) 0.5269 (3) 0.0217 (8)
C9 0.7636 (3) 0.8040 (2) 0.5759 (3) 0.0267 (8)
H9 0.7978 0.7536 0.6008 0.032*
C10 0.8303 (3) 0.8763 (2) 0.5877 (3) 0.0307 (9)
H10 0.9115 0.8743 0.6199 0.037*
C11 0.7829 (3) 0.9500 (2) 0.5545 (3) 0.0295 (9)
C12 0.6644 (3) 0.9517 (2) 0.5073 (3) 0.0341 (9)
H12 0.6292 1.0023 0.4843 0.041*
C13 0.5966 (3) 0.8805 (2) 0.4934 (3) 0.0301 (9)
H13 0.5157 0.8826 0.4605 0.036*
C14 0.8567 (3) 1.0273 (2) 0.5677 (3) 0.0458 (11)
H14A 0.8793 1.0458 0.4989 0.069*
H14B 0.9310 1.0169 0.6139 0.069*
H14C 0.8080 1.0697 0.5989 0.069*
C15 0.8417 (3) 0.6094 (2) 0.3973 (3) 0.0361 (10)
H15A 0.8263 0.6104 0.3206 0.054*
H15C 0.9291 0.6010 0.4164 0.054*
H15B 0.8161 0.6615 0.4264 0.054*
C16 0.8058 (3) 0.45790 (19) 0.3946 (3) 0.0322 (9)
H16A 0.7479 0.4153 0.4115 0.048*
H16C 0.8882 0.4429 0.4239 0.048*
H16B 0.8050 0.4635 0.3182 0.048*
C17 0.7688 (3) 0.5393 (2) 0.4421 (3) 0.0264 (8)
C18 0.5894 (3) 0.5475 (2) 0.3036 (3) 0.0292 (9)
H18A 0.6039 0.4914 0.2783 0.035*
H18B 0.6335 0.5864 0.2610 0.035*
C19 0.4532 (3) 0.5665 (2) 0.2936 (3) 0.0286 (9)
H19B 0.4395 0.6233 0.3167 0.034*
H19A 0.4202 0.5612 0.2193 0.034*
C20 0.2599 (3) 0.5272 (2) 0.3719 (3) 0.0271 (8)
H20 0.2554 0.5804 0.4102 0.033*
C21 0.2064 (3) 0.4599 (2) 0.4382 (3) 0.0284 (9)
H21B 0.1166 0.4606 0.4221 0.034*
H21A 0.2360 0.4069 0.4129 0.034*
C22 0.1847 (3) 0.5349 (2) 0.2649 (3) 0.0393 (10)
H22C 0.2188 0.5788 0.2240 0.059*
H22B 0.0996 0.5477 0.2762 0.059*
H22A 0.1880 0.4832 0.2266 0.059*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.0054 (3) 0.0286 (3) 0.0277 (4) −0.0020 (2) −0.0018 (2) 0.0003 (3)
P1 0.0101 (4) 0.0288 (5) 0.0254 (6) 0.0011 (4) −0.0012 (4) 0.0002 (4)
S1 0.0183 (5) 0.0418 (6) 0.0253 (6) 0.0041 (4) −0.0039 (4) 0.0001 (4)
O1 0.0097 (11) 0.0319 (13) 0.0286 (16) 0.0078 (10) −0.0013 (10) −0.0016 (10)
O2 0.0102 (11) 0.0251 (12) 0.0287 (15) −0.0035 (9) −0.0003 (10) 0.0007 (10)
O3 0.0090 (11) 0.0259 (12) 0.0311 (16) −0.0025 (9) −0.0037 (10) −0.0022 (10)
N1 0.0093 (14) 0.0271 (16) 0.0282 (19) −0.0002 (12) −0.0046 (12) 0.0010 (13)
N2 0.0068 (13) 0.0291 (17) 0.0287 (19) −0.0005 (12) 0.0022 (12) 0.0010 (13)
C1 0.0087 (16) 0.0267 (18) 0.030 (2) 0.0015 (14) −0.0059 (15) −0.0003 (15)
C2 0.0074 (16) 0.037 (2) 0.028 (2) −0.0006 (15) −0.0028 (15) −0.0053 (16)
C3 0.0164 (18) 0.041 (2) 0.025 (2) 0.0003 (16) 0.0000 (16) −0.0053 (16)
C4 0.0109 (17) 0.0274 (19) 0.035 (2) −0.0008 (14) −0.0083 (15) −0.0062 (15)
C5 0.0088 (17) 0.037 (2) 0.037 (3) −0.0005 (15) 0.0000 (16) 0.0045 (17)
C6 0.0208 (19) 0.037 (2) 0.031 (2) 0.0005 (16) 0.0033 (17) 0.0057 (17)
C7 0.0173 (19) 0.053 (3) 0.044 (3) 0.0011 (18) −0.0110 (18) −0.005 (2)
C8 0.0154 (17) 0.0243 (18) 0.025 (2) −0.0019 (14) −0.0005 (15) −0.0022 (14)
C9 0.0120 (17) 0.0276 (19) 0.039 (3) 0.0033 (14) −0.0042 (15) −0.0014 (16)
C10 0.0104 (17) 0.035 (2) 0.045 (3) 0.0011 (15) −0.0036 (16) −0.0060 (18)
C11 0.0216 (19) 0.0244 (19) 0.042 (3) −0.0039 (15) 0.0015 (17) −0.0068 (17)
C12 0.028 (2) 0.0241 (19) 0.049 (3) 0.0052 (16) −0.0078 (18) 0.0010 (17)
C13 0.0134 (17) 0.034 (2) 0.041 (3) 0.0020 (16) −0.0046 (16) 0.0004 (17)
C14 0.033 (2) 0.032 (2) 0.071 (4) −0.0046 (18) 0.002 (2) −0.007 (2)
C15 0.0163 (18) 0.040 (2) 0.052 (3) −0.0080 (17) 0.0056 (18) −0.0021 (19)
C16 0.0117 (17) 0.039 (2) 0.046 (3) −0.0004 (16) 0.0041 (16) −0.0026 (18)
C17 0.0038 (15) 0.032 (2) 0.043 (3) −0.0026 (14) 0.0005 (15) −0.0032 (17)
C18 0.0139 (17) 0.037 (2) 0.038 (3) −0.0031 (15) 0.0064 (16) 0.0042 (17)
C19 0.0194 (18) 0.035 (2) 0.030 (2) 0.0013 (16) −0.0020 (16) 0.0037 (16)
C20 0.0071 (16) 0.038 (2) 0.036 (2) 0.0036 (15) −0.0035 (15) 0.0000 (17)
C21 0.0051 (16) 0.037 (2) 0.043 (3) −0.0018 (15) −0.0024 (15) −0.0024 (17)
C22 0.0195 (19) 0.051 (3) 0.045 (3) 0.0058 (18) −0.0129 (17) 0.004 (2)

Geometric parameters (Å, °)

Ni1—N1 2.076 (3) C9—H9 0.9500
Ni1—N1i 2.076 (3) C10—C11 1.367 (4)
Ni1—N2 2.093 (2) C10—H10 0.9500
Ni1—N2i 2.093 (2) C11—C12 1.388 (4)
Ni1—O3i 2.106 (2) C11—C14 1.504 (4)
Ni1—O3 2.106 (2) C12—C13 1.385 (4)
P1—O3 1.491 (2) C12—H12 0.9500
P1—O1 1.621 (2) C13—H13 0.9500
P1—O2 1.627 (2) C14—H14A 0.9800
P1—S1 1.9372 (14) C14—H14B 0.9800
O1—C1 1.407 (4) C14—H14C 0.9800
O2—C8 1.395 (3) C15—C17 1.535 (4)
N1—C20 1.480 (4) C15—H15A 0.9800
N1—C19 1.485 (4) C15—H15C 0.9800
N1—H1 0.92 (3) C15—H15B 0.9800
N2—C18 1.474 (4) C16—C17 1.533 (4)
N2—C17 1.518 (4) C16—H16A 0.9800
N2—H2 0.96 (3) C16—H16C 0.9800
C1—C2 1.370 (4) C16—H16B 0.9800
C1—C6 1.376 (4) C17—C21i 1.529 (5)
C2—C3 1.384 (4) C18—C19 1.522 (4)
C2—H2A 0.9500 C18—H18A 0.9900
C3—C4 1.399 (4) C18—H18B 0.9900
C3—H3 0.9500 C19—H19B 0.9900
C4—C5 1.382 (5) C19—H19A 0.9900
C4—C7 1.519 (4) C20—C21 1.536 (4)
C5—C6 1.385 (4) C20—C22 1.540 (4)
C5—H5 0.9500 C20—H20 1.0000
C6—H6 0.9500 C21—C17i 1.529 (5)
C7—H7A 0.9800 C21—H21B 0.9900
C7—H7C 0.9800 C21—H21A 0.9900
C7—H7B 0.9800 C22—H22C 0.9800
C8—C13 1.366 (4) C22—H22B 0.9800
C8—C9 1.390 (4) C22—H22A 0.9800
C9—C10 1.392 (4)
N1—Ni1—N1i 180.0 C11—C10—C9 122.2 (3)
N1—Ni1—N2 84.83 (11) C11—C10—H10 118.9
N1i—Ni1—N2 95.17 (11) C9—C10—H10 118.9
N1—Ni1—N2i 95.17 (11) C10—C11—C12 118.1 (3)
N1i—Ni1—N2i 84.83 (11) C10—C11—C14 121.4 (3)
N2—Ni1—N2i 180.0 C12—C11—C14 120.6 (3)
N1—Ni1—O3i 90.54 (10) C13—C12—C11 120.8 (3)
N1i—Ni1—O3i 89.46 (10) C13—C12—H12 119.6
N2—Ni1—O3i 93.63 (9) C11—C12—H12 119.6
N2i—Ni1—O3i 86.37 (9) C8—C13—C12 120.2 (3)
N1—Ni1—O3 89.46 (10) C8—C13—H13 119.9
N1i—Ni1—O3 90.54 (10) C12—C13—H13 119.9
N2—Ni1—O3 86.37 (9) C11—C14—H14A 109.5
N2i—Ni1—O3 93.63 (9) C11—C14—H14B 109.5
O3i—Ni1—O3 179.999 (1) H14A—C14—H14B 109.5
O3—P1—O1 109.22 (12) C11—C14—H14C 109.5
O3—P1—O2 102.67 (12) H14A—C14—H14C 109.5
O1—P1—O2 103.25 (11) H14B—C14—H14C 109.5
O3—P1—S1 120.90 (10) C17—C15—H15A 109.5
O1—P1—S1 107.79 (10) C17—C15—H15C 109.5
O2—P1—S1 111.61 (9) H15A—C15—H15C 109.5
C1—O1—P1 122.1 (2) C17—C15—H15B 109.5
C8—O2—P1 122.6 (2) H15A—C15—H15B 109.5
P1—O3—Ni1 143.74 (12) H15C—C15—H15B 109.5
C20—N1—C19 115.3 (2) C17—C16—H16A 109.5
C20—N1—Ni1 115.0 (2) C17—C16—H16C 109.5
C19—N1—Ni1 105.51 (19) H16A—C16—H16C 109.5
C20—N1—H1 108.7 (19) C17—C16—H16B 109.5
C19—N1—H1 106 (2) H16A—C16—H16B 109.5
Ni1—N1—H1 105 (2) H16C—C16—H16B 109.5
C18—N2—C17 115.9 (2) N2—C17—C21i 108.1 (2)
C18—N2—Ni1 106.15 (18) N2—C17—C16 110.2 (3)
C17—N2—Ni1 121.8 (2) C21i—C17—C16 111.8 (3)
C18—N2—H2 110 (2) N2—C17—C15 108.8 (3)
C17—N2—H2 107.0 (18) C21i—C17—C15 108.2 (3)
Ni1—N2—H2 93.0 (17) C16—C17—C15 109.7 (3)
C2—C1—C6 120.6 (3) N2—C18—C19 107.6 (3)
C2—C1—O1 122.5 (3) N2—C18—H18A 110.2
C6—C1—O1 116.8 (3) C19—C18—H18A 110.2
C1—C2—C3 119.2 (3) N2—C18—H18B 110.2
C1—C2—H2A 120.4 C19—C18—H18B 110.2
C3—C2—H2A 120.4 H18A—C18—H18B 108.5
C2—C3—C4 121.6 (3) N1—C19—C18 109.0 (3)
C2—C3—H3 119.2 N1—C19—H19B 109.9
C4—C3—H3 119.2 C18—C19—H19B 109.9
C5—C4—C3 117.6 (3) N1—C19—H19A 109.9
C5—C4—C7 120.2 (3) C18—C19—H19A 109.9
C3—C4—C7 122.1 (3) H19B—C19—H19A 108.3
C4—C5—C6 121.0 (3) N1—C20—C21 108.9 (3)
C4—C5—H5 119.5 N1—C20—C22 112.0 (3)
C6—C5—H5 119.5 C21—C20—C22 110.3 (3)
C1—C6—C5 120.0 (3) N1—C20—H20 108.5
C1—C6—H6 120.0 C21—C20—H20 108.5
C5—C6—H6 120.0 C22—C20—H20 108.5
C4—C7—H7A 109.5 C17i—C21—C20 120.1 (3)
C4—C7—H7C 109.5 C17i—C21—H21B 107.3
H7A—C7—H7C 109.5 C20—C21—H21B 107.3
C4—C7—H7B 109.5 C17i—C21—H21A 107.3
H7A—C7—H7B 109.5 C20—C21—H21A 107.3
H7C—C7—H7B 109.5 H21B—C21—H21A 106.9
C13—C8—C9 120.3 (3) C20—C22—H22C 109.5
C13—C8—O2 121.1 (3) C20—C22—H22B 109.5
C9—C8—O2 118.6 (3) H22C—C22—H22B 109.5
C8—C9—C10 118.4 (3) C20—C22—H22A 109.5
C8—C9—H9 120.8 H22C—C22—H22A 109.5
C10—C9—H9 120.8 H22B—C22—H22A 109.5
O3—P1—O1—C1 −32.3 (3) C2—C3—C4—C7 177.2 (3)
O2—P1—O1—C1 76.4 (2) C3—C4—C5—C6 0.8 (5)
S1—P1—O1—C1 −165.4 (2) C7—C4—C5—C6 −176.9 (3)
O3—P1—O2—C8 −179.0 (2) C2—C1—C6—C5 −0.4 (5)
O1—P1—O2—C8 67.5 (2) O1—C1—C6—C5 176.8 (3)
S1—P1—O2—C8 −48.0 (2) C4—C5—C6—C1 −0.3 (5)
O1—P1—O3—Ni1 −177.58 (19) P1—O2—C8—C13 −91.2 (4)
O2—P1—O3—Ni1 73.3 (2) P1—O2—C8—C9 91.8 (3)
S1—P1—O3—Ni1 −51.7 (2) C13—C8—C9—C10 −1.4 (5)
N1—Ni1—O3—P1 −144.9 (2) O2—C8—C9—C10 175.6 (3)
N1i—Ni1—O3—P1 35.1 (2) C8—C9—C10—C11 1.2 (5)
N2—Ni1—O3—P1 −60.0 (2) C9—C10—C11—C12 −0.3 (5)
N2i—Ni1—O3—P1 120.0 (2) C9—C10—C11—C14 −179.8 (3)
N2—Ni1—N1—C20 −143.3 (2) C10—C11—C12—C13 −0.6 (6)
N2i—Ni1—N1—C20 36.7 (2) C14—C11—C12—C13 178.9 (3)
O3i—Ni1—N1—C20 123.1 (2) C9—C8—C13—C12 0.6 (5)
O3—Ni1—N1—C20 −56.9 (2) O2—C8—C13—C12 −176.3 (3)
N2—Ni1—N1—C19 −15.08 (19) C11—C12—C13—C8 0.5 (5)
N2i—Ni1—N1—C19 164.92 (19) C18—N2—C17—C21i −173.6 (3)
O3i—Ni1—N1—C19 −108.67 (19) Ni1—N2—C17—C21i −41.9 (3)
O3—Ni1—N1—C19 71.33 (19) C18—N2—C17—C16 −51.1 (4)
N1—Ni1—N2—C18 −15.2 (2) Ni1—N2—C17—C16 80.6 (3)
N1i—Ni1—N2—C18 164.8 (2) C18—N2—C17—C15 69.2 (4)
O3i—Ni1—N2—C18 75.0 (2) Ni1—N2—C17—C15 −159.1 (2)
O3—Ni1—N2—C18 −105.0 (2) C17—N2—C18—C19 −179.2 (3)
N1—Ni1—N2—C17 −150.8 (2) Ni1—N2—C18—C19 42.2 (3)
N1i—Ni1—N2—C17 29.2 (2) C20—N1—C19—C18 170.7 (3)
O3i—Ni1—N2—C17 −60.6 (2) Ni1—N1—C19—C18 42.7 (3)
O3—Ni1—N2—C17 119.4 (2) N2—C18—C19—N1 −58.6 (3)
P1—O1—C1—C2 −52.2 (4) C19—N1—C20—C21 177.5 (3)
P1—O1—C1—C6 130.7 (3) Ni1—N1—C20—C21 −59.3 (3)
C6—C1—C2—C3 0.7 (5) C19—N1—C20—C22 55.2 (4)
O1—C1—C2—C3 −176.3 (3) Ni1—N1—C20—C22 178.4 (2)
C1—C2—C3—C4 −0.3 (5) N1—C20—C21—C17i 79.5 (4)
C2—C3—C4—C5 −0.4 (5) C22—C20—C21—C17i −157.2 (3)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···S1i 0.92 (3) 2.66 (3) 3.574 (3) 171 (3)
N2—H2···O2 0.96 (3) 2.27 (3) 3.234 (3) 178 (3)

Symmetry codes: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2207).

References

  1. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  2. Feng, J.-S., Zou, L.-K., Xie, B., Xiang, Y.-G. & Lai, C. (2010). Acta Cryst. E66, m1593. [DOI] [PMC free article] [PubMed]
  3. He, L.-X., Zou, L.-K., Xie, B., Xiang, Y.-G. & Feng, J.-S. (2010). Acta Cryst. E66, m428. [DOI] [PMC free article] [PubMed]
  4. Pesin, V. G. & Khaletakii, A. M. (1961). J. Gen. Chem. USSR, 31, 2337–2343.
  5. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
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  7. Zou, L.-K., Xie, B., Feng, J.-S. & Lai, C. (2010). Acta Cryst. E66, m1592. [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/S1600536810051184/nc2207sup1.cif

e-67-00m59-sup1.cif (25.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810051184/nc2207Isup2.hkl

e-67-00m59-Isup2.hkl (263.3KB, hkl)

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


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