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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jan 15;67(Pt 2):o398. doi: 10.1107/S1600536811000882

N,N′-Bis(4-amino­benz­yl)oxalamide

Juan Saulo Gonzalez-Gonzalez a, Francisco J Martínez-Martínez a, Efrén V García-Báez b,*, Olivia M Franco-Hernández b, Itzia I Padilla-Martínez b
PMCID: PMC3051624  PMID: 21523071

Abstract

In the title compound, C16H18N4O2, the two carbonyl groups are in an anti­periplanar conformation with an O=C—C=O torsion angle of 173.86 (17)°. In the crystal, a pair of inter­molecular N—H⋯O hydrogen bonds, forming an R 2 2(10) ring motif, connect the mol­ecules into an inversion dimer. The dimers are further linked by N—H⋯N and C—H⋯π inter­actions, forming a zigzag chain along the b axis.

Related literature

For bond-length data, see: Allen et al. (1987). For hydrogen-bond motifs, see: Bernstein et al. (1995). For related structures, see: Lee & Wang (2007). For background to and applications of oxalamides, see: Martínez-Martínez et al. (1998); Padilla-Martínez et al. (2001); Nguyen et al. (2001).graphic file with name e-67-0o398-scheme1.jpg

Experimental

Crystal data

  • C16H18N4O2

  • M r = 298.34

  • Monoclinic, Inline graphic

  • a = 10.7970 (9) Å

  • b = 8.0930 (8) Å

  • c = 17.9888 (7) Å

  • β = 110.151 (10)°

  • V = 1475.7 (2) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 293 K

  • 0.40 × 0.30 × 0.20 mm

Data collection

  • Bruker APEXII area-detector diffractometer

  • 13460 measured reflections

  • 2577 independent reflections

  • 2041 reflections with I > 2σ(I)

  • R int = 0.050

Refinement

  • R[F 2 > 2σ(F 2)] = 0.047

  • wR(F 2) = 0.141

  • S = 1.05

  • 2577 reflections

  • 199 parameters

  • H-atom parameters constrained

  • Δρmax = 0.24 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); 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: SHELXL97 and WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811000882/is2647sup1.cif

e-67-0o398-sup1.cif (22.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811000882/is2647Isup2.hkl

e-67-0o398-Isup2.hkl (124KB, hkl)

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

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

Cg1 is the centroid of the C1–C6 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
N4—H4A⋯N16i 0.86 2.48 3.240 (3) 147
N4—H4B⋯O9ii 0.86 2.35 3.196 (2) 170
N8—H8⋯N4iii 0.86 2.31 3.085 (2) 150
N11—H11⋯O9iv 0.86 2.27 3.015 (2) 145
C6—H6⋯Cg1iii 0.93 2.94 3.836 (3) 162

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

Acknowledgments

The authors gratefully acknowledge financial support from the FRABA-Universidad de Colima, CONACYT 83378 and SIP-IPN.

supplementary crystallographic information

Comment

The chemical structure of oxalamides favors the formation of intra and intermolecular hydrogen bonding interactions (Martínez-Martínez et al., 1998; Padilla-Martínez et al., 2001; Nguyen et al., 2001). Herein we present the title compound, (I), a new bis-oxalamide.

The title compound (I) forms monoclinic crystals (P21/c, Z = 4). Carbonyl groups are antiperiplanar, with an O9—C9—C10—O10 torsion angle of 173.86 (17)°. The oxalamide group is almost planar, with an N8—C9—C10—N11 torsion angle of 171.92 (17)°. The aminobenzyl groups are twisted by 69.43 (5)° (C1—C7/N4) and 73.78 (5)° (C13—C18/N16) out of the oxalamide group mean plane (C7/N8/C9/O9/C10/O10/N11/C12) and are almost parallel to each other with an angle between the planes of 4.56 (5)°. According to graph-set notation (Bernstein et al., 1995), two S(5) rings are formed through N8—H8···O10 and N11—H11···O9 interactions. N···O distances and N—H···O angles are in the range for strong hydrogen bonding, in agreement with similar structures (Lee and Wang, 2007). The zero dimensional array is given by pairing of two molecules through self complementary strong N11—H11···O9 hydrogen bonding, to form the R22(10) motif characteristic of oxalamides. The molecules are connected by N8—H8···N4 and C6—H6···Cg1 into a zigzag chain running along the b axis; Cg1 is the centroid of the C1–C6 ring. Amine N4—H4A···N16 and N4—H4B···O9 hydrogen bonding interactions give the second and third dimensions, forming C(17) and C(10) chains, respectively.

Experimental

A mixture of diethyl oxalate (2 ml,14 mmol) and 4-aminobenzylamine (3.34 ml, 28 mmol) in ethanol (30 ml) was refluxed for 6 h. The suspension was filtered and the resulting solid was washed with cold ethyl alcohol to yield 3.25 g (73%) of a pale yellow solid (m.p. 250–252 °C).

IR (neat, cm-1): 3415, 3346, 3202, 3038, 1651. Anal. calcd. for C16H18N4O2: C 64.41, H 6.08, N 18.78%; found: C 64.07, H 6.25, N 18.44%. 1H NMR (300 MHz, DMSOd-6, δ) CH2 4.11 (d, 2H), NH 9.03 (t, 1H), Aromatics: 6.46 (d, 2H), 6.90 (d, 2H), NH2 4.95 (s, 2H). 13C NMR (75.46 MHz, DMSOd-6, δ) 42.7, 114.2, 126.3, 129.1, 148.3, 160.5. ESI MS = calc. m/z 298.14, found m/z 320.8 [M + Na]+.

Refinement

H atoms bonded to C were positioned geometrically with aromatic C—H = 0.93 Å and aliphatic C—H = 0.97 Å. Their displacement parameters were set at Uiso(H)= 1.2Ueq(C). The amino H atoms were found in a Fourier difference map and refined with the constraints of N—H = 0.86 Å and Uiso(H) = 1.2Ueq(N).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom labeling scheme and 50% probability displacement ellipsoids. Dashed lines indicate intramolecular hydrogen bonding.

Fig. 2.

Fig. 2.

Packing diagram of the title compound, dashed lines indicate intermolecular hydrogen bonding.

Crystal data

C16H18N4O2 F(000) = 632
Mr = 298.34 Dx = 1.343 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 600 reflections
a = 10.7970 (9) Å θ = 20–25°
b = 8.0930 (8) Å µ = 0.09 mm1
c = 17.9888 (7) Å T = 293 K
β = 110.151 (10)° Prism, colorless
V = 1475.7 (2) Å3 0.40 × 0.30 × 0.20 mm
Z = 4

Data collection

Bruker APEXII area-detector diffractometer 2041 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.050
graphite θmax = 25.0°, θmin = 2.4°
φ and ω scans h = −12→12
13460 measured reflections k = −8→9
2577 independent reflections l = −21→21

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)] = 0.047 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.141 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0744P)2 + 0.3652P] where P = (Fo2 + 2Fc2)/3
2577 reflections (Δ/σ)max < 0.001
199 parameters Δρmax = 0.24 e Å3
0 restraints Δρmin = −0.21 e Å3

Special details

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
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)

x y z Uiso*/Ueq
O9 −0.04287 (12) 0.80255 (17) 0.03285 (8) 0.0510 (4)
O10 0.28644 (13) 0.6703 (2) 0.11061 (9) 0.0636 (5)
N4 −0.22384 (17) 0.7608 (2) 0.35278 (10) 0.0581 (6)
N8 0.04232 (14) 0.56568 (19) 0.09827 (9) 0.0439 (5)
N11 0.19920 (15) 0.8886 (2) 0.03145 (9) 0.0478 (5)
N16 0.4741 (2) 0.6082 (3) −0.21045 (14) 0.0872 (9)
C1 −0.12077 (16) 0.5601 (2) 0.16642 (10) 0.0404 (6)
C2 −0.22418 (18) 0.6700 (3) 0.15269 (11) 0.0488 (6)
C3 −0.26137 (18) 0.7320 (3) 0.21331 (11) 0.0505 (7)
C4 −0.19297 (17) 0.6871 (2) 0.29106 (11) 0.0431 (6)
C5 −0.09016 (19) 0.5751 (3) 0.30558 (11) 0.0493 (6)
C6 −0.05570 (18) 0.5125 (3) 0.24415 (11) 0.0488 (6)
C7 −0.08159 (18) 0.4955 (3) 0.09935 (11) 0.0472 (6)
C9 0.05074 (17) 0.7099 (2) 0.06609 (10) 0.0399 (6)
C10 0.19201 (18) 0.7547 (2) 0.07215 (10) 0.0430 (6)
C12 0.3227 (2) 0.9461 (3) 0.02409 (13) 0.0561 (7)
C13 0.36006 (17) 0.8540 (2) −0.03788 (11) 0.0453 (6)
C14 0.45884 (18) 0.7383 (3) −0.01763 (13) 0.0542 (7)
C15 0.4959 (2) 0.6559 (3) −0.07410 (15) 0.0610 (8)
C16 0.4330 (2) 0.6865 (3) −0.15412 (13) 0.0563 (7)
C17 0.3328 (2) 0.8023 (3) −0.17473 (13) 0.0667 (8)
C18 0.2968 (2) 0.8838 (3) −0.11778 (13) 0.0600 (7)
H2 −0.27013 0.70323 0.10101 0.0586*
H3 −0.33254 0.80416 0.20198 0.0606*
H4A −0.28523 0.83393 0.34251 0.0696*
H4B −0.18144 0.73296 0.40102 0.0696*
H5 −0.04405 0.54185 0.35724 0.0591*
H6 0.01287 0.43645 0.25513 0.0586*
H7A −0.15096 0.52059 0.04962 0.0567*
H7B −0.07300 0.37623 0.10376 0.0567*
H8 0.11364 0.51010 0.11973 0.0527*
H11 0.12828 0.94390 0.00844 0.0574*
H12A 0.31459 1.06273 0.01087 0.0673*
H12B 0.39291 0.93392 0.07483 0.0673*
H14A 0.50224 0.71438 0.03561 0.0650*
H15 0.56389 0.57895 −0.05811 0.0732*
H16A 0.43692 0.63146 −0.25982 0.1046*
H16B 0.53677 0.53665 −0.19591 0.1046*
H17 0.28877 0.82581 −0.22794 0.0801*
H18 0.22843 0.96034 −0.13353 0.0720*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O9 0.0456 (7) 0.0494 (8) 0.0576 (8) 0.0014 (6) 0.0173 (6) 0.0056 (6)
O10 0.0457 (8) 0.0741 (10) 0.0721 (10) 0.0067 (7) 0.0219 (7) 0.0212 (8)
N4 0.0659 (11) 0.0607 (11) 0.0553 (10) 0.0091 (9) 0.0308 (9) −0.0015 (8)
N8 0.0436 (8) 0.0456 (9) 0.0468 (9) 0.0005 (7) 0.0212 (7) 0.0029 (7)
N11 0.0457 (9) 0.0467 (9) 0.0575 (9) −0.0019 (7) 0.0261 (7) 0.0031 (8)
N16 0.0781 (13) 0.1039 (18) 0.1004 (16) −0.0224 (13) 0.0575 (12) −0.0310 (14)
C1 0.0394 (9) 0.0395 (10) 0.0437 (10) −0.0073 (7) 0.0163 (8) −0.0001 (8)
C2 0.0422 (10) 0.0619 (13) 0.0405 (10) 0.0012 (9) 0.0119 (8) 0.0086 (9)
C3 0.0406 (10) 0.0573 (12) 0.0553 (12) 0.0093 (9) 0.0187 (9) 0.0087 (10)
C4 0.0428 (10) 0.0425 (10) 0.0489 (10) −0.0055 (8) 0.0220 (8) 0.0014 (8)
C5 0.0525 (11) 0.0547 (12) 0.0403 (10) 0.0066 (9) 0.0156 (8) 0.0079 (9)
C6 0.0480 (10) 0.0468 (11) 0.0526 (11) 0.0088 (9) 0.0186 (9) 0.0036 (9)
C7 0.0497 (10) 0.0462 (11) 0.0500 (11) −0.0096 (9) 0.0226 (9) −0.0050 (9)
C9 0.0432 (10) 0.0431 (10) 0.0362 (9) −0.0010 (8) 0.0173 (8) −0.0044 (8)
C10 0.0442 (10) 0.0477 (11) 0.0399 (9) −0.0013 (9) 0.0179 (8) −0.0017 (8)
C12 0.0536 (12) 0.0529 (12) 0.0691 (13) −0.0151 (9) 0.0305 (10) −0.0055 (10)
C13 0.0384 (9) 0.0474 (11) 0.0541 (11) −0.0074 (8) 0.0210 (8) 0.0058 (9)
C14 0.0426 (10) 0.0638 (13) 0.0574 (12) −0.0010 (10) 0.0187 (9) 0.0143 (10)
C15 0.0513 (12) 0.0529 (13) 0.0876 (16) 0.0037 (10) 0.0351 (11) 0.0096 (12)
C16 0.0477 (11) 0.0610 (13) 0.0701 (14) −0.0178 (10) 0.0329 (10) −0.0091 (11)
C17 0.0548 (12) 0.0921 (18) 0.0524 (12) −0.0055 (12) 0.0174 (10) 0.0059 (12)
C18 0.0485 (11) 0.0689 (14) 0.0639 (13) 0.0098 (10) 0.0210 (10) 0.0134 (11)

Geometric parameters (Å, °)

O9—C9 1.235 (2) C9—C10 1.535 (3)
O10—C10 1.224 (2) C12—C13 1.507 (3)
N4—C4 1.398 (3) C13—C18 1.384 (3)
N8—C7 1.460 (3) C13—C14 1.371 (3)
N8—C9 1.320 (2) C14—C15 1.385 (3)
N11—C10 1.325 (2) C15—C16 1.386 (3)
N11—C12 1.461 (3) C16—C17 1.382 (3)
N16—C16 1.391 (3) C17—C18 1.382 (3)
N4—H4A 0.8600 C2—H2 0.9300
N4—H4B 0.8600 C3—H3 0.9300
N8—H8 0.8600 C5—H5 0.9300
N11—H11 0.8600 C6—H6 0.9300
N16—H16A 0.8600 C7—H7A 0.9700
N16—H16B 0.8600 C7—H7B 0.9700
C1—C6 1.386 (3) C12—H12A 0.9700
C1—C7 1.503 (3) C12—H12B 0.9700
C1—C2 1.382 (3) C14—H14A 0.9300
C2—C3 1.380 (3) C15—H15 0.9300
C3—C4 1.386 (3) C17—H17 0.9300
C4—C5 1.386 (3) C18—H18 0.9300
C5—C6 1.378 (3)
O9···N11 2.713 (2) H2···C14xi 2.9800
O9···N11i 3.015 (2) H2···H7A 2.3500
O9···N4ii 3.196 (2) H2···H14Axi 2.3300
O10···C13 3.382 (2) H3···H4A 2.4100
O10···N8 2.704 (2) H3···C18i 3.0400
O9···H11i 2.2700 H4A···H3 2.4100
O9···H5iii 2.6900 H4A···O10iii 2.8500
O9···H4Bii 2.3500 H4A···H8iii 2.2500
O9···H7A 2.6300 H4A···N16vii 2.4800
O9···H11 2.3400 H4A···C16vii 3.0700
O10···H8 2.3200 H4A···H16Bvii 2.0900
O10···H12B 2.6100 H4B···H5 2.4500
O10···H4Aiv 2.8500 H4B···H8iii 2.4300
O10···H16Bv 2.6000 H4B···O9vi 2.3500
O10···H16Avi 2.8300 H5···H4B 2.4500
O10···H17vi 2.9000 H5···O9iv 2.6900
N4···N8iii 3.085 (2) H5···C9iv 3.0300
N4···O9vi 3.196 (2) H6···C3iv 3.0300
N4···N16vii 3.240 (3) H7A···O9 2.6300
N8···O10 2.704 (2) H7A···H2 2.3500
N8···N4iv 3.085 (2) H7A···C10ix 3.0500
N11···O9i 3.015 (2) H8···O10 2.3200
N11···O9 2.713 (2) H8···N4iv 2.3100
N16···N4viii 3.240 (3) H8···C4iv 3.0300
N4···H16Bvii 2.9300 H8···H4Aiv 2.2500
N4···H8iii 2.3100 H8···H4Biv 2.4300
N16···H4Aviii 2.4800 H11···O9 2.3400
C3···C18i 3.509 (3) H11···O9i 2.2700
C7···C10ix 3.536 (3) H12A···H18 2.5800
C7···C9ix 3.523 (3) H12A···C14x 2.9000
C9···C7ix 3.523 (3) H12A···C15x 3.0100
C10···C7ix 3.536 (3) H12B···O10 2.6100
C12···C14x 3.506 (3) H12B···H14A 2.3700
C13···O10 3.382 (2) H14A···C2xii 3.0000
C14···C15v 3.547 (3) H14A···H2xii 2.3300
C14···C12x 3.506 (3) H14A···H12B 2.3700
C15···C14v 3.547 (3) H14A···C15v 3.0700
C18···C3i 3.509 (3) H14A···H15v 2.5500
C2···H18i 3.0100 H15···H16B 2.4200
C2···H14Axi 3.0000 H15···C14v 2.9600
C3···H18i 2.9600 H15···H14Av 2.5500
C3···H6iii 3.0300 H16A···H17 2.4500
C4···H8iii 3.0300 H16A···O10ii 2.8300
C9···H5iii 3.0300 H16B···H15 2.4200
C10···H7Aix 3.0500 H16B···O10v 2.6000
C14···H2xii 2.9800 H16B···N4viii 2.9300
C14···H15v 2.9600 H16B···H4Aviii 2.0900
C14···H12Ax 2.9000 H17···H16A 2.4500
C15···H14Av 3.0700 H17···O10ii 2.9000
C15···H12Ax 3.0100 H18···H12A 2.5800
C16···H4Aviii 3.0700 H18···C2i 3.0100
C18···H3i 3.0400 H18···C3i 2.9600
C7—N8—C9 123.50 (17) C13—C14—C15 121.9 (2)
C10—N11—C12 122.67 (17) C14—C15—C16 120.9 (2)
H4A—N4—H4B 120.00 N16—C16—C17 122.0 (2)
C4—N4—H4B 120.00 N16—C16—C15 120.7 (2)
C4—N4—H4A 120.00 C15—C16—C17 117.3 (2)
C7—N8—H8 118.00 C16—C17—C18 121.3 (2)
C9—N8—H8 118.00 C13—C18—C17 121.5 (2)
C10—N11—H11 119.00 C1—C2—H2 119.00
C12—N11—H11 119.00 C3—C2—H2 119.00
C16—N16—H16A 120.00 C2—C3—H3 120.00
C16—N16—H16B 120.00 C4—C3—H3 120.00
H16A—N16—H16B 120.00 C4—C5—H5 120.00
C2—C1—C6 117.19 (17) C6—C5—H5 120.00
C6—C1—C7 121.88 (17) C1—C6—H6 119.00
C2—C1—C7 120.93 (16) C5—C6—H6 119.00
C1—C2—C3 122.01 (18) N8—C7—H7A 109.00
C2—C3—C4 120.2 (2) N8—C7—H7B 109.00
N4—C4—C5 121.58 (17) C1—C7—H7A 109.00
C3—C4—C5 118.37 (18) C1—C7—H7B 109.00
N4—C4—C3 119.97 (17) H7A—C7—H7B 108.00
C4—C5—C6 120.60 (18) N11—C12—H12A 109.00
C1—C6—C5 121.6 (2) N11—C12—H12B 109.00
N8—C7—C1 112.83 (17) C13—C12—H12A 109.00
O9—C9—N8 125.51 (18) C13—C12—H12B 109.00
O9—C9—C10 121.24 (15) H12A—C12—H12B 108.00
N8—C9—C10 113.25 (15) C13—C14—H14A 119.00
O10—C10—C9 121.48 (16) C15—C14—H14A 119.00
N11—C10—C9 113.58 (16) C14—C15—H15 120.00
O10—C10—N11 124.94 (19) C16—C15—H15 120.00
N11—C12—C13 113.26 (18) C16—C17—H17 119.00
C12—C13—C18 121.34 (18) C18—C17—H17 119.00
C12—C13—C14 121.55 (18) C13—C18—H18 119.00
C14—C13—C18 117.10 (19) C17—C18—H18 119.00
C7—N8—C9—C10 −179.47 (15) C4—C5—C6—C1 0.8 (3)
C9—N8—C7—C1 −83.4 (2) O9—C9—C10—O10 173.86 (17)
C7—N8—C9—O9 −0.5 (3) O9—C9—C10—N11 −7.1 (2)
C12—N11—C10—O10 3.8 (3) N8—C9—C10—O10 −7.1 (2)
C10—N11—C12—C13 80.5 (2) N8—C9—C10—N11 171.93 (15)
C12—N11—C10—C9 −175.23 (16) N11—C12—C13—C14 −105.0 (2)
C2—C1—C6—C5 −1.6 (3) N11—C12—C13—C18 75.6 (2)
C7—C1—C2—C3 −179.5 (2) C12—C13—C14—C15 −178.5 (2)
C6—C1—C7—N8 −72.8 (2) C18—C13—C14—C15 1.0 (3)
C7—C1—C6—C5 178.5 (2) C12—C13—C18—C17 178.5 (2)
C6—C1—C2—C3 0.6 (3) C14—C13—C18—C17 −0.9 (3)
C2—C1—C7—N8 107.3 (2) C13—C14—C15—C16 −0.6 (4)
C1—C2—C3—C4 1.3 (3) C14—C15—C16—N16 177.4 (2)
C2—C3—C4—N4 174.6 (2) C14—C15—C16—C17 0.2 (4)
C2—C3—C4—C5 −2.1 (3) N16—C16—C17—C18 −177.4 (2)
N4—C4—C5—C6 −175.6 (2) C15—C16—C17—C18 −0.1 (4)
C3—C4—C5—C6 1.1 (3) C16—C17—C18—C13 0.5 (4)

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

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C1–C6 ring.
D—H···A D—H H···A D···A D—H···A
N4—H4A···N16vii 0.86 2.48 3.240 (3) 147
N4—H4B···O9vi 0.86 2.35 3.196 (2) 170
N8—H8···O10 0.86 2.32 2.704 (2) 107
N8—H8···N4iv 0.86 2.31 3.085 (2) 150
N11—H11···O9 0.86 2.34 2.713 (2) 107
N11—H11···O9i 0.86 2.27 3.015 (2) 145
C6—H6···Cg1iv 0.93 2.94 3.836 (3) 162

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IS2647).

References

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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/S1600536811000882/is2647sup1.cif

e-67-0o398-sup1.cif (22.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811000882/is2647Isup2.hkl

e-67-0o398-Isup2.hkl (124KB, hkl)

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


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