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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Nov 24;68(Pt 12):o3431. doi: 10.1107/S1600536812046922

Morpholine-4-carboxamidinium ethyl carbonate

Ioannis Tiritiris a,*
PMCID: PMC3589013  PMID: 23476249

Abstract

The asymmetric unit of the title salt, C5H12N3O+·C3H5O3 , contains two carboxamidinium and two ethyl carbonate ions. In the crystal, the C—N bond lengths in the central CN3 units of the cations range between 1.324 (2) and 1.352 (2) Å, indicating partial double-bond character. The central C atoms are bonded to the three N atoms in a nearly ideal trigonal–planar geometry and the positive charges are delocalized in the CN3 planes. The morpholine rings are in chair conformations. The C—O bond lengths in both ethyl carbonate ions are characteristic for delocalized double bonds [1.243 (2)–1.251 (2) Å] and typical single bonds [1.368 (2) and 1.375 (2) Å]. In the crystal, N—H⋯O hydrogen bonds between cations and anions generate a two-dimensional network in the ac plane.

Related literature  

For the synthesis and crystal structures of guanidinium hydrogen carbonates, see: Tiritiris et al. (2011). For the crystal structure of 4-morpholine­carboxamidine, see: Tiritiris (2012a ). For the crystal structure of piperidine-1-carboxamidinium ethyl carbonate, see: Tiritiris (2012b ).graphic file with name e-68-o3431-scheme1.jpg

Experimental  

Crystal data  

  • C5H12N3O+·C3H5O3

  • M r = 219.25

  • Monoclinic, Inline graphic

  • a = 10.2163 (5) Å

  • b = 20.8874 (9) Å

  • c = 10.4616 (5) Å

  • β = 109.505 (2)°

  • V = 2104.31 (17) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.11 mm−1

  • T = 100 K

  • 0.30 × 0.25 × 0.15 mm

Data collection  

  • Bruker–Nonius KappaCCD diffractometer

  • 9902 measured reflections

  • 5199 independent reflections

  • 2981 reflections with I > 2σ(I)

  • R int = 0.055

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.050

  • wR(F 2) = 0.112

  • S = 1.00

  • 5199 reflections

  • 305 parameters

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

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.30 e Å−3

Data collection: COLLECT (Hooft, 2004); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812046922/kp2441sup1.cif

e-68-o3431-sup1.cif (22.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046922/kp2441Isup2.hkl

e-68-o3431-Isup2.hkl (254.6KB, hkl)

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

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

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H11⋯O4i 0.84 (2) 2.12 (2) 2.944 (1) 168 (1)
N1—H12⋯O3ii 0.89 (2) 1.91 (2) 2.795 (1) 174 (1)
N2—H21⋯O6 0.85 (2) 1.97 (2) 2.807 (1) 168 (1)
N2—H22⋯O4ii 0.92 (2) 1.95 (2) 2.851 (1) 164 (1)
N4—H41⋯O6ii 0.86 (2) 1.97 (2) 2.817 (1) 167 (1)
N4—H42⋯O7i 0.93 (2) 2.00 (2) 2.889 (1) 159 (1)
N5—H51⋯O7ii 0.90 (2) 1.99 (2) 2.879 (1) 172 (1)
N5—H52⋯O3iii 0.90 (2) 1.94 (2) 2.776 (1) 154 (1)

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

Acknowledgments

The author thanks Dr F. Lissner (Institut für Anorganische Chemie, Universität Stuttgart) for the data collection.

supplementary crystallographic information

Comment

The reaction of several guanidines with CO2 in undried aprotic solvents are well described in the literature (Tiritiris et al., 2011). Here, the corresponding guanidinium hydrogen carbonate salts were obtained and their crystal structures could be determined. By reacting carboxamidines with CO2 we first used aprotic solvents and due to their water content, sparingly soluble and non crystalline hydrogen carbonate salts were also formed. By using alcohols as solvents for the reaction, we obtained a few crystalline alkyl carbonate salts. One of them is the here presented title compound. According to the structure analysis, the asymmetric unit contains two carboxamidinium and two ethyl carbonate ions. The C–N bonds of the CN3 units are ranging from 1.324 (2) to 1.352 (2) Å, showing partial double-bond character. The N–C1–N and N–C6–N angles are indicating a nearly ideal trigonal-planar surrounding of the carbon centres by the nitrogen atoms. The positive charges are completely delocalized on the CN3 planes (Fig. 1). The structural parameters of the morpholine rings in the here presented title compound agree very well with the data obtained from the X-ray analysis of the starting compound 4-morpholinecarboxamidine (Tiritiris, 2012a). The morpholine rings adopt a chair conformation. The C–O bond lengths in both ethyl carbonate ions indicate evenly distributed double bonds [1.243 (2)–1.251 (2) Å] and typical single bonds [1.368 (2) and 1.375 (2) Å]. The data fit with the C–O bond lengths and angles of the anion in piperidine-1-carboxamidinium ethyl carbonate (Tiritiris, 2012b). In the crystal structure, strong N—H···O hydrogen bonds between hydrogen atoms of carboxamidinium ions and oxygen atoms of neighboring ethyl carbonate ions are observed, generating an infinite two-dimensional network [d(H···O) = 1.91 (2)–2.12 (2) Å] (Tab. 1) with base vectors [0 0 1] and [1 0 0] (Fig. 2). In contrast to the crystal structure of 4-morpholinecarboxamidine (Tiritiris, 2012a), the oxygen atoms of the morpholine rings are not involved in the N—H···O hydrogen bonding system.

Experimental

The title compound was prepared by bubbling excess CO2 gas into an ethanolic solution of 2.0 g (15.5 mmol) 4-morpholinecarboxamidine (Tiritiris, 2012a). The resulting colorless precipitate was recrystallized from a small amount of ethanol and single crystals suitable for X-ray analysis were obtained. Yield: 3.05 g (90%). 1H NMR (500 MHz, D2O/DSS): δ = 1.17–1.20 [t, 3 H, –CH3], 3.49–3.52 [m, 4 H, –CH2], 3.64–3.68 [q, 2 H, –CH2], 3.80–3.83 [m, 4 H, –CH2]. Because of the H/D exchange, the hydrogen atoms of the –NH2 groups were not observed. 13C NMR (125 MHz, D2O/DSS): δ = 16.8 (–CH3), 45.2 (–CH2), 57.4 (–CH2), 65.4 (–CH2), 156.6 (N3C+), 160.3 (C═O).

Refinement

The N-bound H atoms were located in a difference Fourier map and were refined freely [N—H = 0.84 (2)–0.93 (2) Å]. The hydrogen atoms of the methyl groups were allowed to rotate with a fixed angle around the C–C bond to best fit the experimental electron density, with U(H) set to 1.5 Ueq(C) and d(C—H) = 0.98 Å. The H atoms of the methylene groups were placed in calculated positions with d(C—H) = 0.99 Å. They were included in the refinement in the riding model approximation, with U(H) set to 1.2 Ueq(C).

Figures

Fig. 1.

Fig. 1.

The structure of the title compound with displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

N–H···O hydrogen bonds generating a two-dimensional network in the (ac) plane. The hydrogen bonds are indicated by dashed lines.

Crystal data

C5H12N3O+·C3H5O3 F(000) = 944
Mr = 219.25 Dx = 1.384 Mg m3
Monoclinic, P21/n Melting point: 413 K
Hall symbol: -P 2yn Mo Kα radiation, λ = 0.71073 Å
a = 10.2163 (5) Å Cell parameters from 5142 reflections
b = 20.8874 (9) Å θ = 0.4–28.3°
c = 10.4616 (5) Å µ = 0.11 mm1
β = 109.505 (2)° T = 100 K
V = 2104.31 (17) Å3 Block, colourless
Z = 8 0.30 × 0.25 × 0.15 mm

Data collection

Bruker–Nonius KappaCCD diffractometer 2981 reflections with I > 2σ(I)
Radiation source: sealed tube Rint = 0.055
Graphite monochromator θmax = 28.3°, θmin = 2.3°
φ scans, and ω scans h = −13→13
9902 measured reflections k = −27→27
5199 independent reflections l = −13→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)] = 0.050 Hydrogen site location: difference Fourier map
wR(F2) = 0.112 H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.0468P)2] where P = (Fo2 + 2Fc2)/3
5199 reflections (Δ/σ)max < 0.001
305 parameters Δρmax = 0.25 e Å3
0 restraints Δρmin = −0.30 e Å3

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.

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

x y z Uiso*/Ueq
C1 0.14782 (18) 0.19683 (9) 0.08078 (17) 0.0138 (4)
N1 0.14407 (18) 0.21777 (9) −0.03987 (16) 0.0186 (4)
H11 0.082 (2) 0.2060 (11) −0.111 (2) 0.027 (6)*
H12 0.209 (2) 0.2468 (11) −0.039 (2) 0.028 (6)*
N2 0.24717 (16) 0.21987 (9) 0.18879 (16) 0.0168 (4)
H21 0.2567 (18) 0.2083 (9) 0.269 (2) 0.013 (5)*
H22 0.308 (2) 0.2486 (11) 0.171 (2) 0.032 (6)*
N3 0.05782 (14) 0.15198 (8) 0.09382 (13) 0.0138 (3)
C2 0.04415 (18) 0.14053 (10) 0.22786 (16) 0.0174 (4)
H2A −0.0106 0.1755 0.2491 0.021*
H2B 0.1374 0.1404 0.2982 0.021*
C3 −0.02671 (19) 0.07728 (10) 0.22976 (17) 0.0239 (5)
H3A 0.0343 0.0421 0.2203 0.029*
H3B −0.0410 0.0721 0.3182 0.029*
O1 −0.15763 (13) 0.07261 (7) 0.12343 (12) 0.0227 (3)
C4 −0.13597 (19) 0.07748 (10) −0.00376 (17) 0.0194 (4)
H4A −0.2261 0.0727 −0.0777 0.023*
H4B −0.0746 0.0422 −0.0120 0.023*
C5 −0.07145 (18) 0.14066 (9) −0.01951 (17) 0.0168 (4)
H5A −0.0515 0.1408 −0.1058 0.020*
H5B −0.1379 0.1757 −0.0233 0.020*
C6 0.61678 (17) 0.19115 (9) 0.08546 (16) 0.0122 (4)
N4 0.60204 (17) 0.21566 (9) −0.03589 (15) 0.0161 (4)
H41 0.656 (2) 0.2472 (11) −0.038 (2) 0.026 (6)*
H42 0.533 (2) 0.2013 (12) −0.113 (2) 0.041 (7)*
N5 0.71439 (16) 0.21538 (8) 0.19268 (15) 0.0144 (4)
H51 0.773 (2) 0.2459 (11) 0.185 (2) 0.023 (6)*
H52 0.745 (2) 0.1933 (11) 0.271 (2) 0.035 (6)*
N6 0.53305 (14) 0.14360 (7) 0.10007 (13) 0.0134 (3)
C7 0.56842 (19) 0.11205 (10) 0.23299 (16) 0.0176 (4)
H7A 0.5906 0.1449 0.3053 0.021*
H7B 0.6517 0.0850 0.2480 0.021*
C8 0.4493 (2) 0.07110 (10) 0.24096 (17) 0.0189 (4)
H8A 0.4791 0.0472 0.3277 0.023*
H8B 0.3709 0.0991 0.2401 0.023*
O2 0.40359 (13) 0.02701 (6) 0.13163 (11) 0.0198 (3)
C9 0.35206 (18) 0.06230 (10) 0.00799 (17) 0.0182 (4)
H9A 0.2758 0.0907 0.0117 0.022*
H9B 0.3137 0.0321 −0.0684 0.022*
C10 0.46389 (18) 0.10203 (9) −0.01694 (17) 0.0169 (4)
H10A 0.5335 0.0734 −0.0341 0.020*
H10B 0.4226 0.1288 −0.0986 0.020*
C11 −0.07231 (18) 0.16716 (9) 0.57058 (16) 0.0133 (4)
O3 −0.16622 (12) 0.18499 (7) 0.46539 (11) 0.0196 (3)
O4 −0.04966 (12) 0.18664 (6) 0.68830 (11) 0.0179 (3)
O5 0.01060 (12) 0.11991 (7) 0.54704 (11) 0.0181 (3)
C12 0.12224 (18) 0.09664 (10) 0.66226 (17) 0.0188 (4)
H12A 0.0849 0.0761 0.7281 0.023*
H12B 0.1836 0.1324 0.7081 0.023*
C13 0.20159 (19) 0.04887 (10) 0.60972 (18) 0.0224 (5)
H13A 0.2355 0.0695 0.5427 0.034*
H13B 0.1405 0.0131 0.5671 0.034*
H13C 0.2806 0.0328 0.6851 0.034*
C14 0.40406 (17) 0.17608 (9) 0.57044 (16) 0.0130 (4)
O6 0.31041 (12) 0.19554 (6) 0.46676 (11) 0.0180 (3)
O7 0.42103 (13) 0.19133 (6) 0.69029 (11) 0.0183 (3)
O8 0.49287 (12) 0.13310 (6) 0.54411 (11) 0.0166 (3)
C15 0.60379 (18) 0.10913 (10) 0.65905 (17) 0.0179 (4)
H15A 0.5655 0.0877 0.7232 0.021*
H15B 0.6641 0.1448 0.7070 0.021*
C16 0.68612 (19) 0.06219 (10) 0.60715 (18) 0.0199 (4)
H16A 0.6270 0.0257 0.5651 0.030*
H16B 0.7659 0.0470 0.6828 0.030*
H16C 0.7190 0.0833 0.5398 0.030*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0137 (9) 0.0140 (11) 0.0127 (9) 0.0045 (8) 0.0031 (7) 0.0005 (7)
N1 0.0180 (9) 0.0236 (10) 0.0114 (8) −0.0068 (8) 0.0011 (7) 0.0008 (7)
N2 0.0189 (9) 0.0223 (10) 0.0080 (8) −0.0050 (7) 0.0031 (7) 0.0016 (7)
N3 0.0118 (7) 0.0192 (9) 0.0088 (7) −0.0017 (7) 0.0012 (6) −0.0003 (6)
C2 0.0178 (9) 0.0251 (12) 0.0085 (8) −0.0042 (8) 0.0033 (7) −0.0007 (8)
C3 0.0261 (11) 0.0301 (13) 0.0102 (9) −0.0091 (9) −0.0011 (8) 0.0013 (8)
O1 0.0251 (7) 0.0279 (9) 0.0138 (6) −0.0121 (6) 0.0048 (5) −0.0029 (6)
C4 0.0217 (10) 0.0216 (12) 0.0130 (9) −0.0007 (9) 0.0032 (8) −0.0024 (8)
C5 0.0148 (9) 0.0201 (11) 0.0115 (8) −0.0027 (8) −0.0007 (7) 0.0001 (8)
C6 0.0143 (9) 0.0123 (10) 0.0107 (9) 0.0040 (8) 0.0051 (7) −0.0004 (7)
N4 0.0166 (8) 0.0182 (10) 0.0107 (8) −0.0043 (8) 0.0009 (7) 0.0016 (7)
N5 0.0164 (8) 0.0145 (10) 0.0103 (8) −0.0029 (7) 0.0018 (6) 0.0000 (6)
N6 0.0158 (8) 0.0148 (9) 0.0083 (7) −0.0017 (7) 0.0023 (6) −0.0007 (6)
C7 0.0218 (10) 0.0185 (11) 0.0105 (9) −0.0053 (8) 0.0027 (7) 0.0016 (7)
C8 0.0268 (10) 0.0179 (12) 0.0125 (9) −0.0045 (9) 0.0074 (8) −0.0022 (8)
O2 0.0281 (7) 0.0145 (8) 0.0147 (6) −0.0057 (6) 0.0043 (5) −0.0011 (5)
C9 0.0187 (10) 0.0187 (12) 0.0137 (9) −0.0021 (8) 0.0006 (7) 0.0008 (8)
C10 0.0200 (10) 0.0167 (11) 0.0117 (8) −0.0022 (8) 0.0025 (7) −0.0013 (7)
C11 0.0130 (9) 0.0173 (11) 0.0095 (9) −0.0009 (8) 0.0037 (7) 0.0013 (7)
O3 0.0191 (7) 0.0258 (9) 0.0101 (6) 0.0043 (6) −0.0001 (5) 0.0003 (5)
O4 0.0183 (7) 0.0231 (8) 0.0102 (6) 0.0030 (6) 0.0020 (5) −0.0016 (5)
O5 0.0175 (7) 0.0238 (8) 0.0108 (6) 0.0056 (6) 0.0016 (5) −0.0002 (5)
C12 0.0167 (10) 0.0226 (12) 0.0138 (9) 0.0045 (8) 0.0007 (7) 0.0022 (8)
C13 0.0234 (10) 0.0219 (12) 0.0211 (10) 0.0027 (9) 0.0064 (8) 0.0014 (8)
C14 0.0131 (9) 0.0131 (11) 0.0116 (9) −0.0027 (8) 0.0027 (7) 0.0001 (7)
O6 0.0179 (7) 0.0231 (8) 0.0101 (6) 0.0050 (6) 0.0010 (5) 0.0010 (5)
O7 0.0208 (7) 0.0215 (8) 0.0096 (6) 0.0050 (6) 0.0010 (5) −0.0021 (5)
O8 0.0163 (7) 0.0211 (8) 0.0103 (6) 0.0056 (6) 0.0014 (5) 0.0005 (5)
C15 0.0177 (9) 0.0214 (12) 0.0113 (9) 0.0057 (8) 0.0005 (7) 0.0012 (8)
C16 0.0171 (10) 0.0218 (12) 0.0198 (10) 0.0037 (8) 0.0047 (8) 0.0023 (8)

Geometric parameters (Å, º)

C1—N1 1.324 (2) C7—H7A 0.9900
C1—N2 1.331 (2) C7—H7B 0.9900
C1—N3 1.351 (2) C8—O2 1.420 (2)
N1—H11 0.84 (2) C8—H8A 0.9900
N1—H12 0.89 (2) C8—H8B 0.9900
N2—H21 0.85 (2) O2—C9 1.428 (2)
N2—H22 0.92 (2) C9—C10 1.504 (3)
N3—C5 1.470 (2) C9—H9A 0.9900
N3—C2 1.474 (2) C9—H9B 0.9900
C2—C3 1.510 (3) C10—H10A 0.9900
C2—H2A 0.9900 C10—H10B 0.9900
C2—H2B 0.9900 C11—O4 1.243 (2)
C3—O1 1.429 (2) C11—O3 1.251 (2)
C3—H3A 0.9900 C11—O5 1.375 (2)
C3—H3B 0.9900 O5—C12 1.439 (2)
O1—C4 1.424 (2) C12—C13 1.501 (3)
C4—C5 1.508 (3) C12—H12A 0.9900
C4—H4A 0.9900 C12—H12B 0.9900
C4—H4B 0.9900 C13—H13A 0.9800
C5—H5A 0.9900 C13—H13B 0.9800
C5—H5B 0.9900 C13—H13C 0.9800
C6—N5 1.327 (2) C14—O7 1.248 (2)
C6—N4 1.330 (2) C14—O6 1.2507 (19)
C6—N6 1.352 (2) C14—O8 1.368 (2)
N4—H41 0.86 (2) O8—C15 1.4390 (19)
N4—H42 0.93 (2) C15—C16 1.506 (3)
N5—H51 0.90 (2) C15—H15A 0.9900
N5—H52 0.90 (2) C15—H15B 0.9900
N6—C7 1.471 (2) C16—H16A 0.9800
N6—C10 1.474 (2) C16—H16B 0.9800
C7—C8 1.512 (3) C16—H16C 0.9800
N1—C1—N2 117.44 (18) C8—C7—H7B 109.5
N1—C1—N3 121.41 (16) H7A—C7—H7B 108.0
N2—C1—N3 121.10 (16) O2—C8—C7 112.11 (14)
C1—N1—H11 121.6 (14) O2—C8—H8A 109.2
C1—N1—H12 115.2 (13) C7—C8—H8A 109.2
H11—N1—H12 123.1 (19) O2—C8—H8B 109.2
C1—N2—H21 122.7 (13) C7—C8—H8B 109.2
C1—N2—H22 116.0 (13) H8A—C8—H8B 107.9
H21—N2—H22 121.3 (17) C8—O2—C9 108.51 (14)
C1—N3—C5 119.25 (14) O2—C9—C10 111.74 (14)
C1—N3—C2 119.50 (14) O2—C9—H9A 109.3
C5—N3—C2 113.33 (13) C10—C9—H9A 109.3
N3—C2—C3 110.65 (14) O2—C9—H9B 109.3
N3—C2—H2A 109.5 C10—C9—H9B 109.3
C3—C2—H2A 109.5 H9A—C9—H9B 107.9
N3—C2—H2B 109.5 N6—C10—C9 111.24 (14)
C3—C2—H2B 109.5 N6—C10—H10A 109.4
H2A—C2—H2B 108.1 C9—C10—H10A 109.4
O1—C3—C2 112.19 (15) N6—C10—H10B 109.4
O1—C3—H3A 109.2 C9—C10—H10B 109.4
C2—C3—H3A 109.2 H10A—C10—H10B 108.0
O1—C3—H3B 109.2 O4—C11—O3 127.48 (17)
C2—C3—H3B 109.2 O4—C11—O5 119.35 (15)
H3A—C3—H3B 107.9 O3—C11—O5 113.17 (14)
C4—O1—C3 109.00 (13) C11—O5—C12 117.10 (13)
O1—C4—C5 112.00 (15) O5—C12—C13 106.96 (14)
O1—C4—H4A 109.2 O5—C12—H12A 110.3
C5—C4—H4A 109.2 C13—C12—H12A 110.3
O1—C4—H4B 109.2 O5—C12—H12B 110.3
C5—C4—H4B 109.2 C13—C12—H12B 110.3
H4A—C4—H4B 107.9 H12A—C12—H12B 108.6
N3—C5—C4 111.13 (14) C12—C13—H13A 109.5
N3—C5—H5A 109.4 C12—C13—H13B 109.5
C4—C5—H5A 109.4 H13A—C13—H13B 109.5
N3—C5—H5B 109.4 C12—C13—H13C 109.5
C4—C5—H5B 109.4 H13A—C13—H13C 109.5
H5A—C5—H5B 108.0 H13B—C13—H13C 109.5
N5—C6—N4 118.27 (17) O7—C14—O6 126.70 (17)
N5—C6—N6 120.64 (15) O7—C14—O8 119.38 (14)
N4—C6—N6 121.08 (16) O6—C14—O8 113.91 (14)
C6—N4—H41 116.3 (13) C14—O8—C15 116.75 (12)
C6—N4—H42 121.0 (14) O8—C15—C16 107.70 (14)
H41—N4—H42 122.5 (19) O8—C15—H15A 110.2
C6—N5—H51 121.8 (13) C16—C15—H15A 110.2
C6—N5—H52 120.7 (14) O8—C15—H15B 110.2
H51—N5—H52 114.0 (18) C16—C15—H15B 110.2
C6—N6—C7 118.09 (13) H15A—C15—H15B 108.5
C6—N6—C10 118.98 (14) C15—C16—H16A 109.5
C7—N6—C10 114.80 (15) C15—C16—H16B 109.5
N6—C7—C8 110.93 (14) H16A—C16—H16B 109.5
N6—C7—H7A 109.5 C15—C16—H16C 109.5
C8—C7—H7A 109.5 H16A—C16—H16C 109.5
N6—C7—H7B 109.5 H16B—C16—H16C 109.5
N1—C1—N3—C5 −19.3 (3) N4—C6—N6—C10 23.7 (2)
N2—C1—N3—C5 163.26 (16) C6—N6—C7—C8 167.46 (16)
N1—C1—N3—C2 −166.30 (17) C10—N6—C7—C8 −44.1 (2)
N2—C1—N3—C2 16.3 (3) N6—C7—C8—O2 53.4 (2)
C1—N3—C2—C3 −163.24 (16) C7—C8—O2—C9 −62.83 (19)
C5—N3—C2—C3 47.9 (2) C8—O2—C9—C10 62.98 (19)
N3—C2—C3—O1 −54.7 (2) C6—N6—C10—C9 −167.27 (15)
C2—C3—O1—C4 61.1 (2) C7—N6—C10—C9 44.6 (2)
C3—O1—C4—C5 −60.9 (2) O2—C9—C10—N6 −53.8 (2)
C1—N3—C5—C4 163.03 (16) O4—C11—O5—C12 −1.3 (2)
C2—N3—C5—C4 −48.1 (2) O3—C11—O5—C12 179.62 (15)
O1—C4—C5—N3 54.7 (2) C11—O5—C12—C13 −176.69 (15)
N5—C6—N6—C7 −10.5 (2) O7—C14—O8—C15 −1.3 (2)
N4—C6—N6—C7 170.74 (16) O6—C14—O8—C15 179.56 (15)
N5—C6—N6—C10 −157.57 (16) C14—O8—C15—C16 179.01 (15)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H11···O4i 0.84 (2) 2.12 (2) 2.944 (1) 168 (1)
N1—H12···O3ii 0.89 (2) 1.91 (2) 2.795 (1) 174 (1)
N2—H21···O6 0.85 (2) 1.97 (2) 2.807 (1) 168 (1)
N2—H22···O4ii 0.92 (2) 1.95 (2) 2.851 (1) 164 (1)
N4—H41···O6ii 0.86 (2) 1.97 (2) 2.817 (1) 167 (1)
N4—H42···O7i 0.93 (2) 2.00 (2) 2.889 (1) 159 (1)
N5—H51···O7ii 0.90 (2) 1.99 (2) 2.879 (1) 172 (1)
N5—H52···O3iii 0.90 (2) 1.94 (2) 2.776 (1) 154 (1)

Symmetry codes: (i) x, y, z−1; (ii) x+1/2, −y+1/2, z−1/2; (iii) x+1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KP2441).

References

  1. Brandenburg, K. & Putz, H. (2005). DIAMOND Crystal Impact GbR, D-53002 Bonn, Germany.
  2. Hooft, R. W. W. (2004). COLLECT Bruker–Nonius BV, Delft, The Netherlands.
  3. 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.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Tiritiris, I. (2012a). Acta Cryst. E68, o3118. [DOI] [PMC free article] [PubMed]
  6. Tiritiris, I. (2012b). Acta Cryst. E68, o3310. [DOI] [PMC free article] [PubMed]
  7. Tiritiris, I., Mezger, J., Stoyanov, E. V. & Kantlehner, W. (2011). Z. Naturforsch. Teil B, 66, 407–418.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812046922/kp2441sup1.cif

e-68-o3431-sup1.cif (22.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046922/kp2441Isup2.hkl

e-68-o3431-Isup2.hkl (254.6KB, hkl)

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


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