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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 24;67(Pt 1):o203–o204. doi: 10.1107/S1600536810052670

Bis(2-{2-[2-(benzyl­carbamo­yl)phen­oxy]acetamido}­eth­yl)ammonium nitrate ethanol disolvate

Jiaji Liu a, Xiaoliang Tang a, Zhengdan Lu a, Guolin Zhang a,*, Weisheng Liu a
PMCID: PMC3050242  PMID: 21522705

Abstract

In the title compound, C36H40N5O6 +·NO3 −·2C2H5OH, the nitrate anion is disordered over the two orientations of equal occupancy while the solvent mol­ecule reveals large displacement parameters. The cation is formed by protonation of the N atom of a secondary amine in the middle of the flexible chain and the whole compound has crystallographically imposed C-2 symmetry with the crystallographic b axis. An O atom of the nitrate anion links the acidic H atoms of the cation via N—H⋯O hydrogen bonding. In addition, neighbouring cations are connected by inter­molecular N—H⋯O hydrogen bonds and π–π inter­actions between the benzamide groups of the cations [centroid–centroid distance = 4.000 (3) Å], forming a chain along [001]. The ethanol solvent mol­ecules are arranged on the side of the chain through O—H⋯O hydrogen bonds.

Related literature

Luminescent lanthanide complexes have attracted intense research inter­est due to their very narrow emission bands and large Stokes shifts, see: Wang et al. (2009 ▶); Bunzli & Piguet (2005 ▶); Stein & Wurzberg (1975 ▶). For amide-type open-chain ligands, see: Liu et al. (2009 ▶); Yi et al. (2007 ▶); Hamann et al. (2004 ▶). graphic file with name e-67-0o203-scheme1.jpg

Experimental

Crystal data

  • C36H40N5O6 +·NO3 −·2C2H6O

  • M r = 792.88

  • Monoclinic, Inline graphic

  • a = 16.978 (3) Å

  • b = 11.405 (2) Å

  • c = 11.164 (2) Å

  • β = 108.04 (3)°

  • V = 2055.6 (7) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 296 K

  • 0.22 × 0.18 × 0.17 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1997 ▶) T min = 0.980, T max = 0.984

  • 4901 measured reflections

  • 1995 independent reflections

  • 1334 reflections with I > 2σ(I)

  • R int = 0.035

Refinement

  • R[F 2 > 2σ(F 2)] = 0.063

  • wR(F 2) = 0.190

  • S = 1.03

  • 1995 reflections

  • 277 parameters

  • 45 restraints

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

  • Δρmax = 0.26 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; 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.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810052670/kp2291sup1.cif

e-67-0o203-sup1.cif (23KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052670/kp2291Isup2.hkl

e-67-0o203-Isup2.hkl (98.2KB, 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
N3—HN3⋯O5i 0.95 (4) 2.49 (5) 2.905 (9) 106 (3)
N3—HN3⋯O5ii 0.95 (4) 2.41 (5) 2.905 (9) 112 (3)
N3—HN3⋯O1ii 0.95 (4) 2.01 (4) 2.780 (3) 137 (4)
O4—H4A⋯O3iii 0.85 1.89 2.740 (11) 178
N1—H1A⋯O2 0.86 1.99 2.645 (5) 132
N2—H2A⋯O5ii 0.86 2.14 2.813 (9) 135
N2—H2A⋯O6i 0.86 2.35 3.185 (9) 163

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

This work was supported financially by the National Natural Science Foundation of China (grant Nos. 20771048, 20931003, 21001059) and the Fundamental Research Funds for the Central Universities (lzujbky-2009-k06, lzujbky-2009–114).

supplementary crystallographic information

Comment

Luminescent lanthanide complexes have attracted intense research interest from both material and biological science mainly due to their very narrow emission bands and large Stokes shifts, etc (Wang et al., 2009; Bunzli & Piguet, 2005; Stein & Wurzberg, 1975). Since the lanthanides have low absorptivities and poor quantum yields, fluorescence enhancement has generally been achieved through ligand sensitisation. Among various kinds of ligands, amide type open-chain ligands have drawn much attention in past ten years, mainly due to their flexible structure, selective coordinating capacity and hard binding sites, which could stabilise their lanthanide complexes, acquire novel coordination structure and shield the encapsulated ion from interaction with the surroundings (Liu et al., 2009; Yi et al., 2007; Hamann et al., 2004). There is a need to prepare a new series of amide type ligands to further widen the scope of research on the chemical and physical properties of lanthanide complexes. In this paper, we present the structure of the title compound, a nitrate salt of a free ligand. The asymmetric unit comprises a half of cation C36H40N5O6+ nitrate anion, and ethanol molecule(Fig. 1). In C36H40N5O6+cation, the N atom of secondary amine in the middle of flexible chain is protonated adding more hydrogen bondind donor sites. An O atom of nitrate anion links the acidic H atoms and adjacent one of amide groups via N–H···O hydrogen bonding (Table 1) forming the S-shape organic cation. The carbonyl groups of benzamide at both ends of organic cation are involved in intermolecular N–H···O hydrogen bonds connecting acidic H atoms of neighbouring C36H40N5O6+cations to form a chain. The chain is further stabilised by π–π interactions between the benzamide groups from cations (Fig. 2). Ethanol molecules are arranged on the side of the chain and linked the O atoms of the acetamide groups via O–H···O hydrogen bonds.

Experimental

Ethyl 2-(2-(benzylcarbamoyl)phenoxy)acetate was firstly synthesised as a white solid via a simple prepared by reaction of N-benzylsalicylamide (2.27 g, 10.0 mmol) with ethyl chloroacetate (1.83 g, 15.0 mmol) in 80% yield using an excess amount of anhydrous potassium carbonate in refluxing acetone. Then the ligand, N,N'-iminodiethylenebis{[(2'-benzylaminoformyl)phenoxyl]acetamide}, was obtained in 18% yield by treating the ethyl 2-(2-(benzylcarbamoyl)phenoxy)acetate (1.88 g, 6 mmol) with 0.5 equiv of diethylenetriamine (0.258 g,2.5 mmol) in methanol at 333-338 K for 8 h (m.p. 372-374 K). Single crystals of the title compound suitable for X-ray analysis were obtained by slow evaporation of an ethanol solution (6 mL) containing Tb(NO3)3.6H2O (67.9 mg, 0.15 mmol) and N,N'-iminodiethylenebis{[(2'-benzylaminoformyl)phenoxyl]acetamide} (95.6 mg, 0.15 mmol) after two weeks at room temperature in 75% yield. The preparation was aimed to obtain an Tb(III) nitrate complex with the title ligand but instead the ligand was crystallised.

Refinement

The nitrate group is disordered over two orientations where oxygen atoms of these two orientations revealed occupancies of 0.50 respectively. Furthermore, the anisotropic displacement parameters of the minor occupancy atoms C19, C20 and O4 of ethanol solvent were constrained by using the SHELX command ISOR and SIMU. The ammonium H atoms were located from the difference Fourier map and refined freely. H atoms were positioned geometrically with N—H = 0.86 for amide. All other H atoms were positioned geometrically with C—H = 0.93 and 0.97 Å for aromatic and methylene H atoms, respectively. They were constrained to ride on their parent atoms with Uiso(H)= 1.2Ueq(C) or 1.5 Ueq(C).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound. Displacement ellipsoids are drawn at the 30% probability level. Symmetry code used to generate the complete cation: -x, y, -1 - z.

Fig. 2.

Fig. 2.

The hydrogen bonded chain dominates the crystal packing. Hydrogen bonds are shown as turquiose dashed lines. H atoms not involved in hydrogen bonding have been omitted for clarity. The π···π interactions between benzamide groups are shown as light-blue dashed lines.

Crystal data

C36H40N5O6+·NO3−·2C2H6O F(000) = 844
Mr = 792.88 Dx = 1.281 Mg m−3
Monoclinic, C2 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: C2y Cell parameters from 1019 reflections
a = 16.978 (3) Å θ = 2.5–20.9°
b = 11.405 (2) Å µ = 0.09 mm−1
c = 11.164 (2) Å T = 296 K
β = 108.04 (3)° Block, colourless
V = 2055.6 (7) Å3 0.22 × 0.18 × 0.17 mm
Z = 2

Data collection

Bruker SMART CCD area-detector diffractometer 1995 independent reflections
Radiation source: fine-focus sealed tube 1334 reflections with I > 2σ(I)
graphite Rint = 0.035
φ and ω scans θmax = 25.5°, θmin = 2.2°
Absorption correction: multi-scan (SADABS; Bruker, 1997) h = −20→20
Tmin = 0.980, Tmax = 0.984 k = −13→13
4901 measured reflections l = −8→13

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)] = 0.063 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.190 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.1204P)2] where P = (Fo2 + 2Fc2)/3
1995 reflections (Δ/σ)max < 0.001
277 parameters Δρmax = 0.26 e Å−3
45 restraints Δρmin = −0.32 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 > 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. The structure is non-centrosymmetric with only atoms lighter than silicon, MoKa measured Friedel data can not be used to determine absolute structure.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
C1 0.1027 (3) 0.7751 (5) 0.3251 (4) 0.0729 (14)
H1 0.0513 0.8071 0.2823 0.088*
C2 0.1500 (4) 0.8244 (5) 0.4399 (4) 0.0853 (17)
H2 0.1299 0.8878 0.4742 0.102*
C3 0.2259 (4) 0.7777 (5) 0.5003 (5) 0.0903 (18)
H3 0.2585 0.8102 0.5758 0.108*
C4 0.2544 (4) 0.6830 (6) 0.4502 (5) 0.0860 (17)
H4 0.3060 0.6512 0.4923 0.103*
C5 0.2075 (3) 0.6351 (5) 0.3391 (4) 0.0723 (14)
H5 0.2275 0.5708 0.3062 0.087*
C6 0.1309 (3) 0.6806 (4) 0.2748 (4) 0.0573 (11)
C7 0.0779 (3) 0.6306 (4) 0.1506 (4) 0.0614 (12)
H7A 0.0201 0.6396 0.1453 0.074*
H7B 0.0872 0.6762 0.0828 0.074*
C8 0.0726 (2) 0.4235 (4) 0.1984 (3) 0.0492 (11)
C9 0.0862 (2) 0.2966 (4) 0.1713 (3) 0.0477 (10)
C10 0.0729 (3) 0.2155 (4) 0.2537 (4) 0.0645 (13)
H10 0.0561 0.2411 0.3210 0.077*
C11 0.0839 (4) 0.0971 (5) 0.2393 (5) 0.0802 (16)
H11 0.0741 0.0441 0.2963 0.096*
C12 0.1088 (4) 0.0581 (5) 0.1432 (5) 0.0833 (16)
H12 0.1161 −0.0218 0.1338 0.100*
C13 0.1236 (3) 0.1374 (4) 0.0576 (4) 0.0739 (14)
H13 0.1417 0.1108 −0.0081 0.089*
C14 0.1113 (2) 0.2551 (4) 0.0710 (3) 0.0506 (11)
C15 0.1448 (3) 0.3013 (4) −0.1168 (3) 0.0582 (12)
H15A 0.1031 0.2491 −0.1691 0.070*
H15B 0.1973 0.2602 −0.0900 0.070*
C16 0.1516 (3) 0.4089 (4) −0.1880 (4) 0.0583 (12)
C17 0.1515 (3) 0.4860 (5) −0.3908 (4) 0.0755 (15)
H17A 0.1635 0.4531 −0.4634 0.091*
H17B 0.1978 0.5355 −0.3464 0.091*
C18 0.0744 (3) 0.5599 (4) −0.4352 (4) 0.0633 (12)
H18A 0.0655 0.5993 −0.3635 0.076*
H18B 0.0820 0.6195 −0.4927 0.076*
C19 0.1576 (7) 0.8011 (10) 0.8043 (10) 0.190 (4)
H19A 0.1167 0.7735 0.7280 0.227*
H19B 0.2120 0.7857 0.7965 0.227*
C20 0.1476 (8) 0.9286 (12) 0.8154 (13) 0.220 (5)
H20A 0.0967 0.9441 0.8332 0.330*
H20B 0.1462 0.9660 0.7377 0.330*
H20C 0.1932 0.9589 0.8825 0.330*
N1 0.0936 (2) 0.5070 (3) 0.1313 (3) 0.0555 (9)
H1A 0.1169 0.4881 0.0756 0.067*
N2 0.1437 (2) 0.3914 (4) −0.3083 (3) 0.0627 (10)
H2A 0.1336 0.3217 −0.3385 0.075*
N3 0.0000 0.4879 (5) −0.5000 0.0538 (13)
HN3 −0.004 (2) 0.437 (4) −0.435 (4) 0.061 (12)*
N4 0.0000 0.1418 (5) 0.5000 0.0692 (16)
O1 0.04311 (19) 0.4475 (3) 0.2828 (3) 0.0665 (9)
O2 0.1223 (2) 0.3375 (3) −0.0115 (2) 0.0659 (8)
O3 0.1642 (2) 0.5043 (4) −0.1375 (3) 0.0879 (12)
O4 0.1490 (5) 0.7383 (9) 0.9064 (8) 0.206 (3)
H4A 0.1549 0.6662 0.8924 0.247*
O5 −0.0303 (5) 0.2373 (6) 0.4705 (7) 0.086 (3) 0.50
O6 0.0685 (4) 0.1426 (7) 0.5858 (8) 0.100 (3) 0.50
O7 −0.0314 (6) 0.0489 (6) 0.4703 (11) 0.133 (4) 0.50

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.106 (3) 0.055 (3) 0.059 (2) 0.008 (3) 0.028 (2) 0.008 (2)
C2 0.161 (5) 0.036 (2) 0.068 (3) −0.008 (3) 0.049 (3) −0.002 (2)
C3 0.118 (4) 0.083 (4) 0.061 (3) −0.036 (3) 0.016 (3) 0.004 (3)
C4 0.084 (3) 0.094 (4) 0.073 (3) −0.021 (3) 0.013 (3) 0.002 (3)
C5 0.083 (3) 0.073 (3) 0.062 (3) −0.006 (3) 0.025 (2) −0.003 (2)
C6 0.084 (3) 0.049 (2) 0.0445 (18) 0.001 (2) 0.0277 (19) 0.0087 (18)
C7 0.086 (3) 0.052 (3) 0.046 (2) 0.005 (2) 0.021 (2) 0.0030 (19)
C8 0.056 (2) 0.056 (3) 0.0357 (17) 0.001 (2) 0.0152 (16) −0.0003 (18)
C9 0.057 (2) 0.053 (2) 0.0344 (16) −0.0033 (19) 0.0158 (15) 0.0026 (17)
C10 0.085 (3) 0.066 (3) 0.049 (2) 0.008 (2) 0.030 (2) 0.013 (2)
C11 0.122 (4) 0.068 (3) 0.056 (2) −0.004 (3) 0.035 (3) 0.013 (2)
C12 0.128 (4) 0.052 (3) 0.079 (3) 0.000 (3) 0.046 (3) 0.011 (2)
C13 0.108 (3) 0.063 (3) 0.065 (2) 0.002 (3) 0.048 (2) 0.003 (2)
C14 0.065 (2) 0.050 (2) 0.0426 (19) −0.005 (2) 0.0251 (17) 0.0017 (18)
C15 0.082 (2) 0.063 (3) 0.0391 (17) 0.005 (2) 0.0330 (17) −0.0049 (19)
C16 0.069 (2) 0.066 (3) 0.0455 (19) −0.002 (2) 0.0255 (18) 0.004 (2)
C17 0.076 (2) 0.107 (4) 0.053 (2) 0.004 (3) 0.034 (2) 0.019 (3)
C18 0.090 (3) 0.055 (3) 0.053 (2) −0.015 (2) 0.033 (2) 0.003 (2)
C19 0.183 (6) 0.205 (8) 0.190 (7) −0.004 (7) 0.071 (6) 0.009 (7)
C20 0.218 (7) 0.219 (8) 0.221 (8) −0.005 (7) 0.066 (6) −0.043 (7)
N1 0.075 (2) 0.054 (2) 0.0423 (16) 0.0008 (18) 0.0244 (15) 0.0025 (16)
N2 0.088 (2) 0.067 (2) 0.0447 (16) 0.011 (2) 0.0376 (15) 0.0073 (17)
N3 0.078 (3) 0.051 (3) 0.038 (2) 0.000 0.027 (2) 0.000
N4 0.072 (3) 0.078 (4) 0.069 (3) 0.000 0.038 (3) 0.000
O1 0.0891 (18) 0.070 (2) 0.0545 (14) −0.0011 (17) 0.0420 (14) −0.0032 (15)
O2 0.113 (2) 0.0502 (18) 0.0509 (13) 0.0028 (16) 0.0492 (14) 0.0024 (13)
O3 0.125 (3) 0.080 (2) 0.0584 (17) −0.033 (2) 0.0280 (18) −0.0035 (18)
O4 0.236 (6) 0.214 (7) 0.200 (5) −0.015 (5) 0.117 (5) 0.006 (5)
O5 0.127 (7) 0.065 (4) 0.079 (5) 0.017 (4) 0.049 (5) 0.018 (4)
O6 0.113 (5) 0.063 (5) 0.138 (7) 0.013 (5) 0.061 (5) −0.002 (5)
O7 0.185 (11) 0.070 (5) 0.165 (8) −0.055 (5) 0.084 (7) −0.062 (6)

Geometric parameters (Å, °)

C1—C6 1.367 (7) C16—O3 1.214 (6)
C1—C2 1.402 (7) C16—N2 1.322 (5)
C1—H1 0.9300 C17—N2 1.452 (6)
C2—C3 1.365 (8) C17—C18 1.506 (7)
C2—H2 0.9300 C17—H17A 0.9700
C3—C4 1.371 (8) C17—H17B 0.9700
C3—H3 0.9300 C18—N3 1.493 (5)
C4—C5 1.364 (7) C18—H18A 0.9700
C4—H4 0.9300 C18—H18B 0.9700
C5—C6 1.378 (6) C19—O4 1.392 (11)
C5—H5 0.9300 C19—C20 1.475 (14)
C6—C7 1.512 (6) C19—H19A 0.9700
C7—N1 1.464 (6) C19—H19B 0.9700
C7—H7A 0.9700 C20—H20A 0.9600
C7—H7B 0.9700 C20—H20B 0.9600
C8—O1 1.226 (5) C20—H20C 0.9600
C8—N1 1.327 (5) N1—H1A 0.8600
C8—C9 1.511 (6) N2—H2A 0.8600
C9—C10 1.372 (6) N3—C18i 1.493 (5)
C9—C14 1.398 (5) N3—HN3 0.95 (4)
C10—C11 1.380 (8) N4—O7ii 1.186 (8)
C10—H10 0.9300 N4—O7 1.186 (8)
C11—C12 1.344 (8) N4—O5ii 1.205 (8)
C11—H11 0.9300 N4—O5 1.205 (8)
C12—C13 1.395 (7) N4—O6 1.258 (7)
C12—H12 0.9300 N4—O6ii 1.258 (7)
C13—C14 1.374 (7) O4—H4A 0.8491
C13—H13 0.9300 O5—O5ii 1.035 (14)
C14—O2 1.368 (5) O5—O6ii 1.316 (10)
C15—O2 1.406 (5) O6—O7ii 1.298 (12)
C15—C16 1.486 (6) O6—O5ii 1.316 (10)
C15—H15A 0.9700 O7—O7ii 1.066 (18)
C15—H15B 0.9700 O7—O6ii 1.298 (12)
C6—C1—C2 121.2 (5) O2—C15—H15B 110.3
C6—C1—H1 119.4 C16—C15—H15B 110.3
C2—C1—H1 119.4 H15A—C15—H15B 108.6
C3—C2—C1 118.7 (5) O3—C16—N2 123.7 (4)
C3—C2—H2 120.7 O3—C16—C15 121.6 (4)
C1—C2—H2 120.7 N2—C16—C15 114.8 (4)
C2—C3—C4 120.3 (5) N2—C17—C18 112.6 (4)
C2—C3—H3 119.8 N2—C17—H17A 109.1
C4—C3—H3 119.8 C18—C17—H17A 109.1
C5—C4—C3 120.4 (5) N2—C17—H17B 109.1
C5—C4—H4 119.8 C18—C17—H17B 109.1
C3—C4—H4 119.8 H17A—C17—H17B 107.8
C4—C5—C6 120.9 (5) N3—C18—C17 111.7 (4)
C4—C5—H5 119.5 N3—C18—H18A 109.3
C6—C5—H5 119.5 C17—C18—H18A 109.3
C1—C6—C5 118.5 (4) N3—C18—H18B 109.3
C1—C6—C7 119.3 (4) C17—C18—H18B 109.3
C5—C6—C7 122.2 (4) H18A—C18—H18B 107.9
N1—C7—C6 114.5 (4) O4—C19—C20 113.2 (12)
N1—C7—H7A 108.6 O4—C19—H19A 108.9
C6—C7—H7A 108.6 C20—C19—H19A 108.9
N1—C7—H7B 108.6 O4—C19—H19B 108.9
C6—C7—H7B 108.6 C20—C19—H19B 108.9
H7A—C7—H7B 107.6 H19A—C19—H19B 107.7
O1—C8—N1 121.3 (4) C19—C20—H20A 109.5
O1—C8—C9 119.5 (4) C19—C20—H20B 109.5
N1—C8—C9 119.2 (3) H20A—C20—H20B 109.5
C10—C9—C14 117.6 (4) C19—C20—H20C 109.5
C10—C9—C8 116.4 (4) H20A—C20—H20C 109.5
C14—C9—C8 126.0 (4) H20B—C20—H20C 109.5
C9—C10—C11 121.7 (5) C8—N1—C7 121.0 (4)
C9—C10—H10 119.1 C8—N1—H1A 119.5
C11—C10—H10 119.1 C7—N1—H1A 119.5
C12—C11—C10 120.3 (5) C16—N2—C17 122.1 (4)
C12—C11—H11 119.9 C16—N2—H2A 118.9
C10—C11—H11 119.9 C17—N2—H2A 118.9
C11—C12—C13 120.0 (5) C18—N3—C18i 113.2 (5)
C11—C12—H12 120.0 C18—N3—HN3 102 (2)
C13—C12—H12 120.0 C18i—N3—HN3 117 (2)
C14—C13—C12 119.6 (5) O7ii—N4—O5ii 127.9 (6)
C14—C13—H13 120.2 O7—N4—O5 127.9 (6)
C12—C13—H13 120.2 O7—N4—O6 116.6 (8)
O2—C14—C13 122.8 (4) O5—N4—O6 114.7 (7)
O2—C14—C9 116.4 (4) O7ii—N4—O6ii 116.6 (8)
C13—C14—C9 120.8 (4) O5ii—N4—O6ii 114.7 (7)
O2—C15—C16 106.9 (4) C14—O2—C15 119.3 (3)
O2—C15—H15A 110.3 C19—O4—H4A 107.3
C16—C15—H15A 110.3
C6—C1—C2—C3 1.2 (8) C12—C13—C14—O2 −178.0 (4)
C1—C2—C3—C4 −1.2 (8) C12—C13—C14—C9 1.7 (7)
C2—C3—C4—C5 0.5 (9) C10—C9—C14—O2 178.5 (4)
C3—C4—C5—C6 0.1 (8) C8—C9—C14—O2 −1.8 (5)
C2—C1—C6—C5 −0.5 (7) C10—C9—C14—C13 −1.2 (6)
C2—C1—C6—C7 −179.8 (5) C8—C9—C14—C13 178.5 (4)
C4—C5—C6—C1 −0.1 (7) O2—C15—C16—O3 23.1 (6)
C4—C5—C6—C7 179.2 (5) O2—C15—C16—N2 −157.5 (4)
C1—C6—C7—N1 −155.0 (4) N2—C17—C18—N3 −56.5 (5)
C5—C6—C7—N1 25.7 (7) O1—C8—N1—C7 −3.7 (5)
O1—C8—C9—C10 −7.0 (5) C9—C8—N1—C7 177.2 (3)
N1—C8—C9—C10 172.1 (4) C6—C7—N1—C8 69.5 (5)
O1—C8—C9—C14 173.3 (3) O3—C16—N2—C17 1.6 (7)
N1—C8—C9—C14 −7.6 (5) C15—C16—N2—C17 −177.8 (4)
C14—C9—C10—C11 0.2 (6) C18—C17—N2—C16 −78.9 (5)
C8—C9—C10—C11 −179.6 (4) C17—C18—N3—C18i −169.9 (4)
C9—C10—C11—C12 0.4 (8) C13—C14—O2—C15 1.8 (6)
C10—C11—C12—C13 0.0 (9) C9—C14—O2—C15 −177.9 (3)
C11—C12—C13—C14 −1.1 (8) C16—C15—O2—C14 179.8 (3)

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—HN3···O5iii 0.95 (4) 2.49 (5) 2.905 (9) 106 (3)
N3—HN3···O5iv 0.95 (4) 2.41 (5) 2.905 (9) 112 (3)
N3—HN3···O1iv 0.95 (4) 2.01 (4) 2.780 (3) 137 (4)
O4—H4A···O3v 0.85 1.89 2.740 (11) 178
N1—H1A···O2 0.86 1.99 2.645 (5) 132
N2—H2A···O5iv 0.86 2.14 2.813 (9) 135
N2—H2A···O6iii 0.86 2.35 3.185 (9) 163

Symmetry codes: (iii) x, y, z−1; (iv) −x, y, −z; (v) x, y, z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2291).

References

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  8. Yi, C., Tang, Y., Liu, W. & Tan, M. (2007). Inorg. Chem. Commun. 10, 1505–1509.

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/S1600536810052670/kp2291sup1.cif

e-67-0o203-sup1.cif (23KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052670/kp2291Isup2.hkl

e-67-0o203-Isup2.hkl (98.2KB, hkl)

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


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