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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Dec 15;69(Pt 1):o97. doi: 10.1107/S1600536812050180

Triethyl­ammonium 4-(3,5-dinitro­benzamido)-N-(3,5-dinitro­benzo­yl)benzene­sulfonamidate

Ghulam Waris a, Humaira Masood Siddiqi a,*, Ulrich Flörke b, Rizwan Hussain c, M Saeed Butt a
PMCID: PMC3588331  PMID: 23476476

Abstract

The mol­ecular structure of the title salt, C6H16N+·C20H11N6O12S, shows a planar geometry of the benzamido–phen­yl–sulfonyl moiety, with a dihedral angle of 1.59 (9)° between the aromatic ring planes. The central ring and the aromatic ring of the other dinitro­benzamide group are nearly perpendicular, making a dihedral angle of 89.55 (9)°. All nitro groups lie almost in plane with the associated aromatic rings, the O—N—C—C torsion angles ranging from 9.2 (2) to 24.3 (2)°. In the crystal, strong anion–anion N—H⋯O and anion–cation hydrogen bonds form inversion dimers stacked along the a axis. Less prominent anion–anion C—H⋯O inter­actions lead to the formation of a three-dimensional network including anion–anion dimers as well as anion–anion chains along [100?].

Related literature  

For background to polyamide-imide and other high-temperature resistant polymeric materials, see: Kawakami et al. (2003). For the structure of phthalylsulfacetamide, see: Shin et al. (1984).graphic file with name e-69-00o97-scheme1.jpg

Experimental  

Crystal data  

  • C6H16N+·C20H11N6O12S

  • M r = 661.61

  • Triclinic, Inline graphic

  • a = 9.1046 (12) Å

  • b = 13.2050 (18) Å

  • c = 13.3427 (18) Å

  • α = 98.854 (3)°

  • β = 105.147 (3)°

  • γ = 105.494 (3)°

  • V = 1448.3 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.19 mm−1

  • T = 130 K

  • 0.38 × 0.37 × 0.19 mm

Data collection  

  • Bruker SMART APEX diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2004) T min = 0.931, T max = 0.965

  • 13859 measured reflections

  • 6875 independent reflections

  • 4652 reflections with I > 2σ(I)

  • R int = 0.032

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.084

  • S = 0.89

  • 6875 reflections

  • 415 parameters

  • H-atom parameters constrained

  • Δρmax = 0.36 e Å−3

  • Δρmin = −0.36 e Å−3

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); 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 and local programs.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812050180/pv2607sup1.cif

e-69-00o97-sup1.cif (27KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050180/pv2607Isup2.hkl

e-69-00o97-Isup2.hkl (336.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812050180/pv2607Isup3.cml

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—H1A⋯O8i 0.88 2.00 2.8611 (17) 165
N100—H10P⋯O2ii 0.93 1.86 2.747 (2) 158
C13—H13A⋯O8i 0.95 2.22 3.136 (2) 162
C3—H3A⋯O8i 0.95 2.45 3.221 (2) 139
C6—H6A⋯O11iii 0.95 2.38 3.215 (2) 147
C9—H9A⋯O10iv 0.95 2.48 3.384 (2) 159
C20—H20A⋯O3v 0.95 2.31 3.225 (2) 163

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

Acknowledgments

The authors acknowledge the Higher Education Commission of Pakistan for providing financial assistance for this project through the Inter­national Research Support Initiative Programe (IRSIP) and the Department of Chemistry, Quaid-i-Azam University Islamabad for providing research facilities.

supplementary crystallographic information

Comment

In the past decade, the demand for polyamide-imide (PAI) and other high-temperature resistant polymeric materials has grown progressively because of their outstanding mechanical properties, excellent thermal stability (Kawakami et al., 2003), etc. The title compound is a starting material for such types of materials.

Experimental

In this preparation reagent grade quality chemicals were used without their further purification. In a 100 ml, three necked, round bottomed flask, equipped with a condenser, a nitrogen gas inlet tube, a thermometer and a magnetic stirrer, of sulfanilamide (1.39 g, 0.0086 mole) in dry dichloromethane (20 ml) and a few drops of N,N-dimethylformamide(DMF) stirred at 273–278 K for 30 minutes and 3,5- dinitrobenzoylchloride (3.72 g, 0.0161 mol) in dichloromethane (30 ml) was added dropwise by dropping funnel and stirring was continued for further 1 h under the same conditions. The reaction mixture was then refluxed for 45 min. The flask content was cooled to room temperature, poured into water and let it stand for 24 h. The resulting dark brown precipitates were filtered, washed with hot water and 5% NaOH solution. Finally, the product was washed with hot water and dried under vacuum at 350 K. The crude product was recrystallized from N,N-dimethylformamide(DMF). Yield: 87%; m.p 460–462 K.

Refinement

Hydrogen atoms were clearly identified in difference syntheses, refined at idealized positions riding on the carbon or nitrogen atoms with C—H 0.95–0.98 Å, N—H 0.88 and 0.93 Å and with isotropic displacement parameters Uiso(H) = 1.2Ueq(C/N) or 1.5Ueq(methyl C). All methyl hydrogen atoms were allowed to rotate but not to tip.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound with anisotropic displacement parameters drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Packing diagram viewed along the a-axis showing N–H···O hydrogen bonding pattern as dashed lines. H-atoms not involved are omitted.

Crystal data

C6H16N+·C20H11N6O12S Z = 2
Mr = 661.61 F(000) = 688
Triclinic, P1 Dx = 1.517 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.1046 (12) Å Cell parameters from 2907 reflections
b = 13.2050 (18) Å θ = 2.4–26.9°
c = 13.3427 (18) Å µ = 0.19 mm1
α = 98.854 (3)° T = 130 K
β = 105.147 (3)° Prism, colourless
γ = 105.494 (3)° 0.38 × 0.37 × 0.19 mm
V = 1448.3 (3) Å3

Data collection

Bruker SMART APEX diffractometer 6875 independent reflections
Radiation source: sealed tube 4652 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.032
φ and ω scans θmax = 27.9°, θmin = 1.6°
Absorption correction: multi-scan (SADABS; Sheldrick, 2004) h = −11→10
Tmin = 0.931, Tmax = 0.965 k = −17→17
13859 measured reflections l = −17→17

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)] = 0.041 Hydrogen site location: difference Fourier map
wR(F2) = 0.084 H-atom parameters constrained
S = 0.89 w = 1/[σ2(Fo2) + (0.029P)2] where P = (Fo2 + 2Fc2)/3
6875 reflections (Δ/σ)max = 0.001
415 parameters Δρmax = 0.36 e Å3
0 restraints Δρmin = −0.36 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
S1 0.90395 (6) 0.28292 (3) 0.21593 (4) 0.01914 (11)
O1 1.03295 (15) 0.36565 (9) 0.20308 (10) 0.0246 (3)
O2 0.76199 (15) 0.23599 (9) 0.12131 (9) 0.0245 (3)
O3 0.52517 (16) 0.33418 (9) 0.59254 (11) 0.0317 (3)
O4 0.32249 (17) 0.35984 (10) 0.89035 (11) 0.0385 (4)
O5 0.29330 (18) 0.51042 (11) 0.95560 (12) 0.0435 (4)
O6 0.62662 (18) 0.84333 (10) 0.90660 (12) 0.0426 (4)
O7 0.67579 (18) 0.83485 (10) 0.75614 (12) 0.0404 (4)
O8 1.15593 (14) 0.29259 (9) 0.40479 (9) 0.0214 (3)
O9 0.90468 (16) −0.26946 (9) 0.35110 (11) 0.0317 (3)
O10 0.73408 (15) −0.18561 (9) 0.29762 (10) 0.0275 (3)
O11 1.40360 (16) −0.02522 (10) 0.63169 (10) 0.0315 (3)
O12 1.53041 (14) 0.11153 (9) 0.58183 (10) 0.0248 (3)
N1 0.69344 (17) 0.47991 (11) 0.56319 (11) 0.0187 (3)
H1A 0.7360 0.5508 0.5846 0.022*
N2 0.34552 (19) 0.45696 (13) 0.89879 (12) 0.0266 (4)
N3 0.62909 (19) 0.79268 (12) 0.82266 (14) 0.0279 (4)
N4 0.95176 (17) 0.18180 (11) 0.25028 (11) 0.0191 (3)
N5 0.87053 (19) −0.18774 (11) 0.33830 (12) 0.0214 (4)
N6 1.40938 (18) 0.03787 (11) 0.57313 (12) 0.0208 (3)
C1 0.8402 (2) 0.34117 (13) 0.31860 (13) 0.0169 (4)
C2 0.8728 (2) 0.45227 (13) 0.34808 (13) 0.0188 (4)
H2A 0.9308 0.4983 0.3136 0.023*
C3 0.8206 (2) 0.49557 (13) 0.42770 (14) 0.0185 (4)
H3A 0.8421 0.5716 0.4474 0.022*
C4 0.7365 (2) 0.42858 (13) 0.47979 (14) 0.0173 (4)
C5 0.7027 (2) 0.31665 (13) 0.44911 (14) 0.0201 (4)
H5A 0.6452 0.2702 0.4836 0.024*
C6 0.7535 (2) 0.27417 (13) 0.36838 (14) 0.0201 (4)
H6A 0.7289 0.1980 0.3465 0.024*
C7 0.5933 (2) 0.43160 (13) 0.61400 (14) 0.0189 (4)
C8 0.5640 (2) 0.50400 (13) 0.70085 (14) 0.0176 (4)
C9 0.4789 (2) 0.45188 (14) 0.76106 (14) 0.0193 (4)
H9A 0.4461 0.3752 0.7488 0.023*
C10 0.4427 (2) 0.51314 (14) 0.83887 (14) 0.0199 (4)
C11 0.4892 (2) 0.62476 (14) 0.86136 (14) 0.0220 (4)
H11A 0.4637 0.6657 0.9155 0.026*
C12 0.5748 (2) 0.67311 (13) 0.80072 (15) 0.0209 (4)
C13 0.6110 (2) 0.61631 (13) 0.72018 (14) 0.0198 (4)
H13A 0.6670 0.6531 0.6786 0.024*
C14 1.0699 (2) 0.20335 (13) 0.34280 (14) 0.0176 (4)
C15 1.0969 (2) 0.10340 (13) 0.37607 (13) 0.0166 (4)
C16 0.9761 (2) 0.00384 (13) 0.33703 (14) 0.0174 (4)
H16A 0.8773 −0.0044 0.2848 0.021*
C17 1.0032 (2) −0.08325 (13) 0.37609 (14) 0.0168 (4)
C18 1.1434 (2) −0.07612 (13) 0.45135 (14) 0.0186 (4)
H18A 1.1593 −0.1370 0.4768 0.022*
C19 1.2601 (2) 0.02450 (13) 0.48797 (13) 0.0170 (4)
C20 1.2409 (2) 0.11451 (13) 0.45224 (13) 0.0170 (4)
H20A 1.3243 0.1823 0.4792 0.020*
N100 0.22811 (19) 0.79060 (12) 0.08484 (12) 0.0261 (4)
H10P 0.2155 0.7935 0.0140 0.031*
C101 0.1711 (3) 0.87782 (16) 0.13073 (18) 0.0390 (6)
H10A 0.2443 0.9491 0.1326 0.047*
H10B 0.1762 0.8753 0.2053 0.047*
C102 0.0024 (3) 0.8674 (2) 0.0680 (2) 0.0595 (7)
H10C −0.0289 0.9261 0.1014 0.089*
H10D −0.0711 0.7976 0.0670 0.089*
H10E −0.0029 0.8717 −0.0055 0.089*
C103 0.1294 (3) 0.67768 (15) 0.08118 (17) 0.0356 (5)
H10F 0.0170 0.6640 0.0370 0.043*
H10G 0.1708 0.6253 0.0455 0.043*
C104 0.1301 (3) 0.65733 (18) 0.18919 (19) 0.0483 (6)
H10H 0.0635 0.5827 0.1804 0.072*
H10I 0.0867 0.7076 0.2246 0.072*
H10J 0.2404 0.6685 0.2329 0.072*
C105 0.4047 (2) 0.81232 (17) 0.13686 (16) 0.0355 (5)
H10K 0.4334 0.7480 0.1117 0.043*
H10L 0.4280 0.8243 0.2153 0.043*
C106 0.5073 (3) 0.91023 (18) 0.11218 (17) 0.0456 (6)
H10M 0.6212 0.9213 0.1476 0.068*
H10N 0.4809 0.9744 0.1383 0.068*
H10O 0.4863 0.8982 0.0347 0.068*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0226 (3) 0.0190 (2) 0.0165 (2) 0.00746 (18) 0.0059 (2) 0.00580 (18)
O1 0.0280 (8) 0.0239 (7) 0.0267 (8) 0.0091 (6) 0.0123 (6) 0.0122 (6)
O2 0.0251 (8) 0.0297 (7) 0.0161 (7) 0.0102 (6) 0.0017 (6) 0.0040 (5)
O3 0.0382 (9) 0.0167 (7) 0.0389 (9) 0.0000 (6) 0.0229 (7) 0.0002 (6)
O4 0.0561 (10) 0.0260 (8) 0.0365 (9) 0.0065 (7) 0.0256 (8) 0.0098 (6)
O5 0.0544 (11) 0.0416 (9) 0.0526 (10) 0.0203 (8) 0.0401 (9) 0.0142 (8)
O6 0.0566 (11) 0.0248 (8) 0.0472 (10) 0.0089 (7) 0.0299 (8) −0.0048 (7)
O7 0.0565 (10) 0.0213 (7) 0.0529 (10) 0.0103 (7) 0.0336 (9) 0.0116 (7)
O8 0.0245 (7) 0.0144 (6) 0.0221 (7) 0.0037 (5) 0.0052 (6) 0.0039 (5)
O9 0.0339 (8) 0.0145 (7) 0.0436 (9) 0.0064 (6) 0.0071 (7) 0.0098 (6)
O10 0.0194 (8) 0.0227 (7) 0.0343 (8) 0.0022 (6) 0.0048 (6) 0.0043 (6)
O11 0.0352 (8) 0.0266 (7) 0.0286 (8) 0.0061 (6) 0.0020 (7) 0.0155 (6)
O12 0.0196 (7) 0.0195 (7) 0.0305 (8) 0.0026 (5) 0.0051 (6) 0.0044 (6)
N1 0.0228 (9) 0.0109 (7) 0.0210 (8) 0.0035 (6) 0.0074 (7) 0.0021 (6)
N2 0.0263 (10) 0.0307 (9) 0.0228 (9) 0.0073 (7) 0.0088 (8) 0.0081 (7)
N3 0.0250 (10) 0.0209 (8) 0.0377 (11) 0.0072 (7) 0.0131 (8) 0.0020 (8)
N4 0.0223 (9) 0.0173 (7) 0.0180 (8) 0.0080 (6) 0.0051 (7) 0.0045 (6)
N5 0.0262 (10) 0.0159 (8) 0.0207 (9) 0.0032 (7) 0.0096 (7) 0.0034 (6)
N6 0.0239 (9) 0.0171 (8) 0.0210 (9) 0.0072 (6) 0.0064 (7) 0.0037 (6)
C1 0.0172 (10) 0.0182 (9) 0.0136 (9) 0.0068 (7) 0.0010 (8) 0.0036 (7)
C2 0.0200 (10) 0.0185 (9) 0.0169 (10) 0.0047 (7) 0.0041 (8) 0.0069 (7)
C3 0.0197 (10) 0.0128 (8) 0.0204 (10) 0.0038 (7) 0.0030 (8) 0.0048 (7)
C4 0.0150 (9) 0.0178 (9) 0.0168 (10) 0.0054 (7) 0.0018 (8) 0.0037 (7)
C5 0.0209 (10) 0.0171 (9) 0.0232 (10) 0.0051 (7) 0.0083 (8) 0.0068 (8)
C6 0.0232 (10) 0.0143 (9) 0.0222 (10) 0.0063 (7) 0.0057 (8) 0.0049 (7)
C7 0.0167 (10) 0.0169 (9) 0.0208 (10) 0.0042 (7) 0.0039 (8) 0.0039 (7)
C8 0.0147 (9) 0.0175 (9) 0.0180 (10) 0.0049 (7) 0.0022 (8) 0.0029 (7)
C9 0.0168 (10) 0.0178 (9) 0.0205 (10) 0.0042 (7) 0.0024 (8) 0.0045 (7)
C10 0.0156 (10) 0.0251 (10) 0.0179 (10) 0.0050 (7) 0.0045 (8) 0.0067 (8)
C11 0.0201 (10) 0.0239 (10) 0.0213 (10) 0.0084 (8) 0.0058 (8) 0.0027 (8)
C12 0.0181 (10) 0.0170 (9) 0.0260 (11) 0.0064 (7) 0.0048 (8) 0.0032 (8)
C13 0.0176 (10) 0.0184 (9) 0.0232 (10) 0.0047 (7) 0.0073 (8) 0.0052 (8)
C14 0.0178 (10) 0.0161 (9) 0.0220 (10) 0.0051 (7) 0.0108 (8) 0.0056 (7)
C15 0.0205 (10) 0.0163 (9) 0.0151 (9) 0.0058 (7) 0.0091 (8) 0.0041 (7)
C16 0.0186 (10) 0.0182 (9) 0.0171 (9) 0.0070 (7) 0.0078 (8) 0.0035 (7)
C17 0.0200 (10) 0.0134 (8) 0.0165 (10) 0.0031 (7) 0.0089 (8) 0.0009 (7)
C18 0.0254 (11) 0.0153 (9) 0.0193 (10) 0.0081 (7) 0.0114 (8) 0.0059 (7)
C19 0.0171 (10) 0.0199 (9) 0.0149 (9) 0.0067 (7) 0.0055 (8) 0.0045 (7)
C20 0.0206 (10) 0.0153 (8) 0.0164 (10) 0.0046 (7) 0.0096 (8) 0.0030 (7)
N100 0.0316 (10) 0.0294 (9) 0.0178 (9) 0.0109 (7) 0.0082 (8) 0.0051 (7)
C101 0.0514 (15) 0.0340 (12) 0.0410 (14) 0.0219 (11) 0.0225 (12) 0.0080 (10)
C102 0.0512 (18) 0.0747 (19) 0.076 (2) 0.0408 (15) 0.0293 (15) 0.0307 (15)
C103 0.0432 (14) 0.0290 (11) 0.0350 (13) 0.0087 (10) 0.0163 (11) 0.0073 (9)
C104 0.0536 (16) 0.0516 (15) 0.0494 (16) 0.0169 (12) 0.0232 (13) 0.0281 (12)
C105 0.0306 (13) 0.0507 (14) 0.0224 (12) 0.0139 (10) 0.0034 (10) 0.0080 (10)
C106 0.0334 (14) 0.0634 (16) 0.0289 (13) 0.0030 (11) 0.0069 (11) 0.0072 (11)

Geometric parameters (Å, º)

S1—O1 1.4421 (12) C10—C11 1.381 (2)
S1—O2 1.4584 (12) C11—C12 1.376 (2)
S1—N4 1.6053 (14) C11—H11A 0.9500
S1—C1 1.7708 (18) C12—C13 1.377 (2)
O3—C7 1.2203 (19) C13—H13A 0.9500
O4—N2 1.2251 (18) C14—C15 1.515 (2)
O5—N2 1.2255 (19) C15—C16 1.388 (2)
O6—N3 1.2218 (19) C15—C20 1.389 (2)
O7—N3 1.2253 (19) C16—C17 1.387 (2)
O8—C14 1.2468 (19) C16—H16A 0.9500
O9—N5 1.2242 (18) C17—C18 1.373 (2)
O10—N5 1.2288 (18) C18—C19 1.381 (2)
O11—N6 1.2272 (17) C18—H18A 0.9500
O12—N6 1.2245 (17) C19—C20 1.383 (2)
N1—C7 1.358 (2) C20—H20A 0.9500
N1—C4 1.410 (2) N100—C101 1.496 (2)
N1—H1A 0.8800 N100—C105 1.502 (2)
N2—C10 1.474 (2) N100—C103 1.507 (2)
N3—C12 1.479 (2) N100—H10P 0.9300
N4—C14 1.340 (2) C101—C102 1.503 (3)
N5—C17 1.481 (2) C101—H10A 0.9900
N6—C19 1.474 (2) C101—H10B 0.9900
C1—C2 1.387 (2) C102—H10C 0.9800
C1—C6 1.388 (2) C102—H10D 0.9800
C2—C3 1.379 (2) C102—H10E 0.9800
C2—H2A 0.9500 C103—C104 1.505 (3)
C3—C4 1.399 (2) C103—H10F 0.9900
C3—H3A 0.9500 C103—H10G 0.9900
C4—C5 1.397 (2) C104—H10H 0.9800
C5—C6 1.379 (2) C104—H10I 0.9800
C5—H5A 0.9500 C104—H10J 0.9800
C6—H6A 0.9500 C105—C106 1.517 (3)
C7—C8 1.511 (2) C105—H10K 0.9900
C8—C9 1.389 (2) C105—H10L 0.9900
C8—C13 1.391 (2) C106—H10M 0.9800
C9—C10 1.380 (2) C106—H10N 0.9800
C9—H9A 0.9500 C106—H10O 0.9800
O1—S1—O2 114.78 (8) O8—C14—C15 116.86 (16)
O1—S1—N4 114.71 (8) N4—C14—C15 113.96 (14)
O2—S1—N4 105.36 (7) C16—C15—C20 120.30 (15)
O1—S1—C1 108.37 (8) C16—C15—C14 120.81 (16)
O2—S1—C1 106.53 (8) C20—C15—C14 118.73 (15)
N4—S1—C1 106.51 (8) C17—C16—C15 118.37 (17)
C7—N1—C4 126.94 (14) C17—C16—H16A 120.8
C7—N1—H1A 116.5 C15—C16—H16A 120.8
C4—N1—H1A 116.5 C18—C17—C16 123.38 (16)
O4—N2—O5 123.33 (16) C18—C17—N5 118.55 (15)
O4—N2—C10 118.61 (15) C16—C17—N5 118.00 (16)
O5—N2—C10 118.05 (15) C17—C18—C19 116.22 (16)
O6—N3—O7 124.04 (16) C17—C18—H18A 121.9
O6—N3—C12 118.00 (16) C19—C18—H18A 121.9
O7—N3—C12 117.95 (15) C18—C19—C20 123.31 (17)
C14—N4—S1 116.77 (12) C18—C19—N6 118.34 (15)
O9—N5—O10 124.93 (14) C20—C19—N6 118.28 (15)
O9—N5—C17 117.63 (16) C19—C20—C15 118.41 (15)
O10—N5—C17 117.43 (14) C19—C20—H20A 120.8
O12—N6—O11 124.18 (16) C15—C20—H20A 120.8
O12—N6—C19 118.27 (14) C101—N100—C105 112.12 (15)
O11—N6—C19 117.55 (14) C101—N100—C103 114.20 (16)
C2—C1—C6 119.86 (16) C105—N100—C103 112.11 (15)
C2—C1—S1 120.83 (13) C101—N100—H10P 105.9
C6—C1—S1 119.30 (13) C105—N100—H10P 105.9
C3—C2—C1 119.70 (16) C103—N100—H10P 105.9
C3—C2—H2A 120.2 N100—C101—C102 112.84 (18)
C1—C2—H2A 120.2 N100—C101—H10A 109.0
C2—C3—C4 120.64 (16) C102—C101—H10A 109.0
C2—C3—H3A 119.7 N100—C101—H10B 109.0
C4—C3—H3A 119.7 C102—C101—H10B 109.0
C5—C4—C3 119.39 (16) H10A—C101—H10B 107.8
C5—C4—N1 123.68 (15) C101—C102—H10C 109.5
C3—C4—N1 116.91 (15) C101—C102—H10D 109.5
C6—C5—C4 119.44 (16) H10C—C102—H10D 109.5
C6—C5—H5A 120.3 C101—C102—H10E 109.5
C4—C5—H5A 120.3 H10C—C102—H10E 109.5
C5—C6—C1 120.93 (16) H10D—C102—H10E 109.5
C5—C6—H6A 119.5 C104—C103—N100 114.20 (17)
C1—C6—H6A 119.5 C104—C103—H10F 108.7
O3—C7—N1 123.77 (16) N100—C103—H10F 108.7
O3—C7—C8 118.86 (16) C104—C103—H10G 108.7
N1—C7—C8 117.37 (14) N100—C103—H10G 108.7
C9—C8—C13 119.55 (16) H10F—C103—H10G 107.6
C9—C8—C7 116.10 (15) C103—C104—H10H 109.5
C13—C8—C7 124.31 (16) C103—C104—H10I 109.5
C10—C9—C8 119.00 (16) H10H—C104—H10I 109.5
C10—C9—H9A 120.5 C103—C104—H10J 109.5
C8—C9—H9A 120.5 H10H—C104—H10J 109.5
C9—C10—C11 123.09 (16) H10I—C104—H10J 109.5
C9—C10—N2 118.65 (15) N100—C105—C106 112.26 (17)
C11—C10—N2 118.23 (16) N100—C105—H10K 109.2
C12—C11—C10 115.99 (16) C106—C105—H10K 109.2
C12—C11—H11A 122.0 N100—C105—H10L 109.2
C10—C11—H11A 122.0 C106—C105—H10L 109.2
C11—C12—C13 123.60 (16) H10K—C105—H10L 107.9
C11—C12—N3 118.04 (16) C105—C106—H10M 109.5
C13—C12—N3 118.36 (16) C105—C106—H10N 109.5
C12—C13—C8 118.73 (16) H10M—C106—H10N 109.5
C12—C13—H13A 120.6 C105—C106—H10O 109.5
C8—C13—H13A 120.6 H10M—C106—H10O 109.5
O8—C14—N4 129.16 (16) H10N—C106—H10O 109.5
O1—S1—N4—C14 59.63 (15) O7—N3—C12—C11 −165.52 (17)
O2—S1—N4—C14 −173.15 (13) O6—N3—C12—C13 −165.24 (17)
C1—S1—N4—C14 −60.25 (14) O7—N3—C12—C13 13.8 (2)
O1—S1—C1—C2 20.61 (16) C11—C12—C13—C8 −2.4 (3)
O2—S1—C1—C2 −103.39 (14) N3—C12—C13—C8 178.36 (15)
N4—S1—C1—C2 144.52 (14) C9—C8—C13—C12 1.5 (3)
O1—S1—C1—C6 −160.73 (13) C7—C8—C13—C12 178.89 (16)
O2—S1—C1—C6 75.26 (15) S1—N4—C14—O8 −4.3 (3)
N4—S1—C1—C6 −36.83 (16) S1—N4—C14—C15 173.89 (11)
C6—C1—C2—C3 0.8 (2) O8—C14—C15—C16 156.24 (16)
S1—C1—C2—C3 179.47 (14) N4—C14—C15—C16 −22.2 (2)
C1—C2—C3—C4 0.6 (3) O8—C14—C15—C20 −19.3 (2)
C2—C3—C4—C5 −1.2 (3) N4—C14—C15—C20 162.27 (15)
C2—C3—C4—N1 177.44 (16) C20—C15—C16—C17 0.1 (2)
C7—N1—C4—C5 −11.5 (3) C14—C15—C16—C17 −175.36 (15)
C7—N1—C4—C3 169.93 (16) C15—C16—C17—C18 −0.1 (3)
C3—C4—C5—C6 0.3 (3) C15—C16—C17—N5 176.81 (14)
N1—C4—C5—C6 −178.26 (16) O9—N5—C17—C18 −20.4 (2)
C4—C5—C6—C1 1.2 (3) O10—N5—C17—C18 158.70 (16)
C2—C1—C6—C5 −1.7 (3) O9—N5—C17—C16 162.53 (15)
S1—C1—C6—C5 179.59 (14) O10—N5—C17—C16 −18.3 (2)
C4—N1—C7—O3 −0.3 (3) C16—C17—C18—C19 0.2 (3)
C4—N1—C7—C8 −179.45 (15) N5—C17—C18—C19 −176.71 (15)
O3—C7—C8—C9 9.1 (2) C17—C18—C19—C20 −0.3 (3)
N1—C7—C8—C9 −171.69 (15) C17—C18—C19—N6 176.70 (15)
O3—C7—C8—C13 −168.29 (17) O12—N6—C19—C18 156.51 (16)
N1—C7—C8—C13 10.9 (3) O11—N6—C19—C18 −24.3 (2)
C13—C8—C9—C10 0.1 (3) O12—N6—C19—C20 −26.3 (2)
C7—C8—C9—C10 −177.50 (16) O11—N6—C19—C20 152.85 (16)
C8—C9—C10—C11 −1.0 (3) C18—C19—C20—C15 0.3 (3)
C8—C9—C10—N2 177.07 (15) N6—C19—C20—C15 −176.66 (15)
O4—N2—C10—C9 11.8 (2) C16—C15—C20—C19 −0.2 (2)
O5—N2—C10—C9 −169.00 (17) C14—C15—C20—C19 175.33 (15)
O4—N2—C10—C11 −170.03 (16) C105—N100—C101—C102 170.41 (18)
O5—N2—C10—C11 9.2 (2) C103—N100—C101—C102 −60.7 (2)
C9—C10—C11—C12 0.3 (3) C101—N100—C103—C104 −62.2 (2)
N2—C10—C11—C12 −177.79 (16) C105—N100—C103—C104 66.7 (2)
C10—C11—C12—C13 1.4 (3) C101—N100—C105—C106 −67.0 (2)
C10—C11—C12—N3 −179.29 (15) C103—N100—C105—C106 163.00 (17)
O6—N3—C12—C11 15.4 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1A···O8i 0.88 2.00 2.8611 (17) 165
N100—H10P···O2ii 0.93 1.86 2.747 (2) 158
C13—H13A···O8i 0.95 2.22 3.136 (2) 162
C3—H3A···O8i 0.95 2.45 3.221 (2) 139
C6—H6A···O11iii 0.95 2.38 3.215 (2) 147
C9—H9A···O10iv 0.95 2.48 3.384 (2) 159
C20—H20A···O3v 0.95 2.31 3.225 (2) 163

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2607).

References

  1. Bruker (2002). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Kawakami, H., Nakajima, K., Shimizu, H. & Nagaoka, S. (2003). J. Membr. Sci 212, 195–203.
  3. Sheldrick, G. M. (2004). SADABS University of Göttingen, Germany.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Shin, W., Kim, Y. C. & Koo, C. H. (1984). Bull. Korean Chem. Soc. 5, 23–26.

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/S1600536812050180/pv2607sup1.cif

e-69-00o97-sup1.cif (27KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050180/pv2607Isup2.hkl

e-69-00o97-Isup2.hkl (336.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812050180/pv2607Isup3.cml

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


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