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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Feb 20;69(Pt 3):o398–o399. doi: 10.1107/S1600536813004352

N,N-Diethyl­anilinium 5-(5-chloro-2,4-dinitro­phen­yl)-2,6-dioxo-1,2,3,6-tetra­hydro­pyrimidin-4-olate

R Babykala a, D Kalaivani a,*
PMCID: PMC3588430  PMID: 23476581

Abstract

In the anion of the title salt, C10H16N+·C10H4ClN4O7 [trivial name = N,N-diethyl­anilinium 5-(3-chloro-4,6,-dinitro­phen­yl)barbiturate], the dihedral angle between the benzene and pyrimidine rings is 45.49 (6)°. The mean plane of the nitro group, which is ortho-substituted with respect to the pyrimidine ring, is twisted by 41.57 (13)° from the benzene ring, while the mean plane of the nitro group, which is para-substituted, is twisted by 14.41 (12)° from this ring. In the crystal, N—H⋯O hydrogen bonds link cations and anions into chains along [1-10]. Within the chains, inversion-related anionic barbiturate anions form R 2 2(8) ring motifs.

Related literature  

For different types of inter­actions between electron-deficient nitro aromatics and bases, see: Jackson & Gazzolo (1900); Mulliken (1952); Russell & Janzen (1962); Blake et al. (1966). For donor–acceptor inter­actions see: Mulliken (1952); Radha et al. (1987). For π–π stacking inter­actions, see: Vembu & Fronczek (2009). For the biological activity of pyrimidine and barbiturate derivatives, see: Jain et al. (2006); Tripathi (2009) and of related barbiturates, see: Kalaivani & Buvaneswari (2010). For the crystal structures of related barbiturates, see: Kalaivani & Malarvizhi (2009); Buvaneswari & Kalaivani (2011); Kalaivani & Mangaiyarkarasi (2013). For hydrogen-bond graph-set motifs, see: Bernstein et al. (1995).graphic file with name e-69-0o398-scheme1.jpg

Experimental  

Crystal data  

  • C10H16N+·C10H4ClN4O7

  • M r = 477.86

  • Triclinic, Inline graphic

  • a = 9.8040 (2) Å

  • b = 10.2870 (2) Å

  • c = 11.8260 (2) Å

  • α = 74.727 (1)°

  • β = 82.761 (1)°

  • γ = 71.817 (1)°

  • V = 1091.87 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.23 mm−1

  • T = 293 K

  • 0.30 × 0.30 × 0.20 mm

Data collection  

  • Bruker Kappa APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2004) T min = 0.913, T max = 0.985

  • 18678 measured reflections

  • 3836 independent reflections

  • 3123 reflections with I > 2σ(I)

  • R int = 0.027

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.042

  • wR(F 2) = 0.117

  • S = 1.04

  • 3836 reflections

  • 312 parameters

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

  • Δρmax = 0.40 e Å−3

  • Δρmin = −0.25 e Å−3

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813004352/lh5583sup1.cif

e-69-0o398-sup1.cif (30.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813004352/lh5583Isup2.hkl

e-69-0o398-Isup2.hkl (188KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813004352/lh5583Isup3.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
N4—H4A⋯O5i 0.83 (2) 2.06 (2) 2.892 (2) 175 (2)
N3—H3A⋯O7ii 0.83 (2) 1.96 (2) 2.794 (2) 180 (3)
N5—H5A⋯O6iii 0.87 (3) 1.82 (3) 2.677 (2) 168 (3)

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

Acknowledgments

The authors are thankful to the SAIF, IIT Madras, for the data collection.

supplementary crystallographic information

Comment

Several types of interactions have been observed between electron deficient nitro aromatic compounds and electron rich species (Jackson et al., 1900; Mulliken, 1952; Russell et al., 1962; Blake et al., 1966). Partial transfer of electrons results in the formation of charge-transfer complexes (Mulliken, 1952; Russell et al., 1962). N,N-diethylaniline usually forms charge transfer complexes with electron deficient nitroaromatics which is revealed through the existence of π···π stacking in single crystal X-ray diffraction studies (Vembu et al.,2009). The title molecular salt is formed upon mixing 1,3-dichloro-4,6-dinitrobenzene (DCDNB), N,N-diethylaniline and barbituric acid in which no significant π···π stacking is observed between nitro aromatic ring and N,N-diethylaniline ring. Barbituric acid (pyrimidine-2,4,6(1H,3H,5H)-trione) and many other pyrimidine derivatives occupy a distinct and unique place in everyday life (Jain et al., 2006). Barbiturates are mainly used to stop convulsion and they also have hypnotic property which is applied for the treatment of psychotic patients, induction of state of sleep and prolonged sleep (Tripathi et al., 2009). The related barbiturates synthesised in our laboratory also possess such properties (Kalaivani & Malarvizhi 2009; Kalaivani & Buvaneswari 2010). Single crystal X-ray analysis of the molecular salts derived from (1-chloro-2,4-dinitrobenzene/2,4,6-trinitrobenzene), N,N-diethylaniline and barbituric acid have already been reported by our group (Buvaneswari & Kalaivani 2011; Kalaivani & Mangaiyarkarasi, 2013).

The molecular structure of the title compound is shown in Fig 1. In the crystal, N—H···O hyrogen bonds link cations and anions into chains (Fig 2) along [110] which incorporate R22(8) rings (Bernstein et al., 1995).

Experimental

Analytical grade 1,3-dichloro-4,6-dinitrobenzene (DCDNB) and Barbituric acid (BBA) were used as supplied by Aldrich company. N,N-Diethylaniline was distilled under reduced pressure and the fraction boiling over at its boiling point was used. DCDNB (2.37g, 0.01mol) in 15ml of absolute ethanol was mixed with barbituric acid (1.28g, 0.01mol)in 30ml of absolute ethanol. N,N-diethylaniline (3g, 0.01mol) was added to the above mixture, heated to 313K, and shaken well for 5-6 hrs. The solution was kept at room temperature. After a period of two weeks dark reddish orange block-shaped crystals formed in the solution. The crystals were powdered well and washed with 2 to 5ml of ethanol and 50ml of dry ether and recrystallized from absolute alcohol (m.pt :494K ; yield :80 %). Good quality crystals (dark reddish-orange blocks) for single crystal X-ray studies were obtained by slow evaporation of ethanol solution of the title compound at room temperature.

Refinement

The N-bound H atoms were located in difference Fourier maps and refind independently with isotropic displacement parameters. The C-bound hydrogen atoms were placed in calculated positions and refined as riding atoms: C—H = 0.93, 0.97 and 0.96 Å for CH, CH2 and CH3 H atoms, respectively, with Uiso(H) = k Ueq(C), where k = 1.5 for methyl H atoms and = 1.2 for other H atoms.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound showing 30% probability displacement ellipsoids.

Fig. 2.

Fig. 2.

Part of the crystal structure showing the N—H···O hydrogen bonds as dotted lines.

Crystal data

C10H16N+·C10H4ClN4O7 Z = 2
Mr = 477.86 F(000) = 496
Triclinic, P1 Dx = 1.453 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.8040 (2) Å Cell parameters from 7243 reflections
b = 10.2870 (2) Å θ = 2.2–27.2°
c = 11.8260 (2) Å µ = 0.23 mm1
α = 74.727 (1)° T = 293 K
β = 82.761 (1)° Block, red
γ = 71.817 (1)° 0.30 × 0.30 × 0.20 mm
V = 1091.87 (4) Å3

Data collection

Bruker Kappa APEXII CCD diffractometer 3836 independent reflections
Radiation source: fine-focus sealed tube 3123 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.027
ω and φ scans θmax = 25.0°, θmin = 2.2°
Absorption correction: multi-scan (SADABS; Bruker, 2004) h = −11→11
Tmin = 0.913, Tmax = 0.985 k = −12→12
18678 measured reflections l = −14→14

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)] = 0.042 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0503P)2 + 0.5116P] where P = (Fo2 + 2Fc2)/3
3836 reflections (Δ/σ)max < 0.001
312 parameters Δρmax = 0.40 e Å3
0 restraints Δρmin = −0.25 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 0.0071 (2) 0.0230 (2) −0.27529 (19) 0.0475 (5)
C2 −0.0626 (2) 0.1317 (2) −0.36552 (17) 0.0474 (5)
C3 −0.0487 (2) 0.2634 (2) −0.38156 (17) 0.0477 (5)
H3 −0.0941 0.3359 −0.4425 0.057*
C4 0.0321 (2) 0.2889 (2) −0.30787 (17) 0.0415 (4)
C5 0.10006 (18) 0.18534 (19) −0.21224 (16) 0.0374 (4)
C6 0.0869 (2) 0.0517 (2) −0.20168 (18) 0.0436 (5)
H6 0.1341 −0.0218 −0.1421 0.052*
C7 0.16905 (19) 0.21325 (18) −0.12259 (16) 0.0377 (4)
C8 0.09802 (19) 0.33217 (19) −0.07694 (17) 0.0402 (4)
C9 0.2870 (2) 0.2669 (2) 0.05867 (18) 0.0449 (5)
N4 0.35173 (17) 0.15462 (17) 0.01261 (15) 0.0415 (4)
C11 0.3494 (3) 0.6406 (4) −0.1188 (2) 0.0874 (9)
H11A 0.3532 0.5436 −0.1072 0.131*
H11B 0.2542 0.6937 −0.0985 0.131*
H11C 0.4167 0.6476 −0.0699 0.131*
C12 0.3870 (3) 0.6980 (3) −0.2442 (2) 0.0762 (8)
H12A 0.3780 0.7973 −0.2564 0.091*
H12B 0.3196 0.6896 −0.2933 0.091*
C13 0.5808 (3) 0.6803 (3) −0.4067 (2) 0.0747 (7)
H13A 0.6680 0.6141 −0.4293 0.090*
H13B 0.5059 0.6876 −0.4564 0.090*
C14 0.6049 (6) 0.8165 (4) −0.4284 (4) 0.1406 (17)
H14A 0.5165 0.8850 −0.4140 0.211*
H14B 0.6384 0.8432 −0.5085 0.211*
H14C 0.6756 0.8117 −0.3770 0.211*
C15 0.5662 (2) 0.4699 (3) −0.25663 (18) 0.0520 (5)
C16 0.6740 (2) 0.3853 (3) −0.1841 (2) 0.0589 (6)
H16 0.7297 0.4241 −0.1523 0.071*
C17 0.6985 (3) 0.2419 (3) −0.1592 (2) 0.0736 (7)
H17 0.7704 0.1825 −0.1093 0.088*
C18 0.6163 (4) 0.1865 (3) −0.2085 (3) 0.0808 (8)
H18 0.6332 0.0894 −0.1922 0.097*
C19 0.5097 (4) 0.2736 (4) −0.2812 (3) 0.0837 (9)
H19 0.4546 0.2352 −0.3138 0.100*
C20 0.4836 (3) 0.4154 (3) −0.3062 (2) 0.0694 (7)
H20 0.4113 0.4745 −0.3559 0.083*
N1 0.0461 (2) 0.43164 (19) −0.33939 (16) 0.0544 (5)
N2 −0.1569 (2) 0.1174 (3) −0.44496 (18) 0.0654 (6)
N3 0.16215 (17) 0.35220 (18) 0.01183 (15) 0.0448 (4)
C10 0.29895 (19) 0.11832 (18) −0.07495 (16) 0.0371 (4)
N5 0.5380 (2) 0.6221 (2) −0.28078 (16) 0.0585 (5)
O1 0.16331 (19) 0.44533 (19) −0.33559 (18) 0.0795 (6)
O2 −0.05941 (19) 0.52979 (17) −0.37394 (16) 0.0724 (5)
O3 −0.2340 (2) 0.2254 (3) −0.50262 (19) 0.1009 (7)
O4 −0.1558 (3) 0.0024 (3) −0.4513 (2) 0.1051 (8)
O5 0.37052 (14) 0.00914 (13) −0.10491 (13) 0.0484 (4)
O6 0.33802 (18) 0.28916 (18) 0.13834 (16) 0.0726 (5)
O7 −0.01956 (14) 0.41850 (15) −0.10903 (13) 0.0552 (4)
Cl1 −0.00919 (8) −0.14432 (7) −0.24327 (7) 0.0795 (2)
H4A 0.429 (3) 0.103 (2) 0.0413 (19) 0.050 (6)*
H3A 0.120 (2) 0.420 (2) 0.0409 (19) 0.047 (6)*
H5A 0.590 (3) 0.644 (3) −0.238 (2) 0.072 (8)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0400 (10) 0.0530 (12) 0.0561 (12) −0.0093 (9) −0.0074 (9) −0.0267 (10)
C2 0.0352 (10) 0.0704 (14) 0.0425 (11) −0.0100 (9) −0.0085 (8) −0.0266 (10)
C3 0.0382 (10) 0.0651 (13) 0.0339 (10) −0.0044 (9) −0.0105 (8) −0.0107 (9)
C4 0.0354 (9) 0.0466 (11) 0.0399 (10) −0.0052 (8) −0.0075 (8) −0.0114 (8)
C5 0.0287 (9) 0.0419 (10) 0.0396 (10) 0.0003 (7) −0.0082 (7) −0.0157 (8)
C6 0.0381 (10) 0.0426 (11) 0.0487 (11) −0.0008 (8) −0.0153 (8) −0.0153 (9)
C7 0.0334 (9) 0.0368 (9) 0.0419 (10) −0.0009 (7) −0.0133 (8) −0.0138 (8)
C8 0.0341 (9) 0.0396 (10) 0.0461 (11) −0.0008 (8) −0.0134 (8) −0.0150 (8)
C9 0.0386 (10) 0.0433 (11) 0.0538 (12) 0.0008 (8) −0.0175 (9) −0.0212 (9)
N4 0.0323 (8) 0.0398 (9) 0.0508 (10) 0.0047 (7) −0.0198 (7) −0.0178 (7)
C11 0.0686 (17) 0.111 (2) 0.0614 (17) 0.0041 (16) −0.0067 (13) −0.0204 (16)
C12 0.0681 (16) 0.0864 (19) 0.0613 (16) 0.0003 (14) −0.0242 (13) −0.0135 (14)
C13 0.0782 (18) 0.098 (2) 0.0536 (14) −0.0369 (16) −0.0194 (13) −0.0061 (13)
C14 0.221 (5) 0.109 (3) 0.104 (3) −0.084 (3) −0.027 (3) 0.008 (2)
C15 0.0459 (11) 0.0741 (15) 0.0426 (11) −0.0209 (11) −0.0023 (9) −0.0205 (10)
C16 0.0425 (11) 0.0852 (17) 0.0492 (13) −0.0135 (11) −0.0030 (10) −0.0218 (12)
C17 0.0590 (15) 0.0819 (19) 0.0656 (16) −0.0052 (14) 0.0084 (12) −0.0170 (14)
C18 0.090 (2) 0.0781 (19) 0.0766 (19) −0.0345 (17) 0.0293 (17) −0.0260 (16)
C19 0.096 (2) 0.104 (2) 0.0735 (19) −0.059 (2) 0.0094 (17) −0.0305 (17)
C20 0.0633 (15) 0.101 (2) 0.0587 (15) −0.0389 (14) −0.0094 (12) −0.0222 (14)
N1 0.0529 (11) 0.0553 (11) 0.0509 (11) −0.0123 (9) −0.0147 (9) −0.0040 (8)
N2 0.0491 (11) 0.1064 (18) 0.0543 (12) −0.0243 (12) −0.0102 (9) −0.0363 (12)
N3 0.0387 (9) 0.0413 (9) 0.0558 (10) 0.0053 (7) −0.0188 (8) −0.0267 (8)
C10 0.0336 (9) 0.0348 (9) 0.0431 (10) −0.0032 (8) −0.0125 (8) −0.0127 (8)
N5 0.0554 (11) 0.0807 (14) 0.0446 (10) −0.0206 (10) −0.0213 (9) −0.0142 (10)
O1 0.0631 (11) 0.0739 (12) 0.1013 (14) −0.0317 (9) −0.0211 (10) 0.0015 (10)
O2 0.0740 (11) 0.0520 (9) 0.0756 (12) −0.0005 (8) −0.0290 (9) 0.0018 (8)
O3 0.0875 (14) 0.1337 (19) 0.0848 (14) −0.0213 (13) −0.0548 (12) −0.0209 (13)
O4 0.1107 (17) 0.1282 (19) 0.1117 (18) −0.0526 (15) −0.0386 (14) −0.0513 (15)
O5 0.0393 (7) 0.0416 (7) 0.0634 (9) 0.0081 (6) −0.0221 (6) −0.0258 (7)
O6 0.0622 (10) 0.0751 (11) 0.0873 (12) 0.0129 (8) −0.0443 (9) −0.0515 (10)
O7 0.0417 (8) 0.0527 (8) 0.0684 (10) 0.0147 (6) −0.0284 (7) −0.0320 (7)
Cl1 0.0822 (5) 0.0605 (4) 0.1107 (6) −0.0254 (3) −0.0314 (4) −0.0274 (4)

Geometric parameters (Å, º)

C1—C6 1.381 (3) C12—H12B 0.9700
C1—C2 1.391 (3) C13—C14 1.444 (4)
C1—Cl1 1.716 (2) C13—N5 1.511 (3)
C2—C3 1.365 (3) C13—H13A 0.9700
C2—N2 1.462 (3) C13—H13B 0.9700
C3—C4 1.371 (3) C14—H14A 0.9600
C3—H3 0.9300 C14—H14B 0.9600
C4—C5 1.404 (3) C14—H14C 0.9600
C4—N1 1.463 (3) C15—C16 1.368 (3)
C5—C6 1.392 (3) C15—C20 1.376 (3)
C5—C7 1.458 (2) C15—N5 1.457 (3)
C6—H6 0.9300 C16—C17 1.375 (4)
C7—C8 1.412 (2) C16—H16 0.9300
C7—C10 1.417 (2) C17—C18 1.376 (4)
C8—O7 1.247 (2) C17—H17 0.9300
C8—N3 1.379 (2) C18—C19 1.367 (4)
C9—O6 1.222 (2) C18—H18 0.9300
C9—N3 1.348 (2) C19—C20 1.356 (4)
C9—N4 1.350 (2) C19—H19 0.9300
N4—C10 1.392 (2) C20—H20 0.9300
N4—H4A 0.83 (2) N1—O1 1.208 (2)
C11—C12 1.490 (4) N1—O2 1.222 (2)
C11—H11A 0.9600 N2—O4 1.201 (3)
C11—H11B 0.9600 N2—O3 1.215 (3)
C11—H11C 0.9600 N3—H3A 0.83 (2)
C12—N5 1.511 (3) C10—O5 1.239 (2)
C12—H12A 0.9700 N5—H5A 0.87 (3)
C6—C1—C2 118.98 (19) C14—C13—H13B 108.7
C6—C1—Cl1 117.21 (16) N5—C13—H13B 108.7
C2—C1—Cl1 123.67 (16) H13A—C13—H13B 107.6
C3—C2—C1 119.82 (17) C13—C14—H14A 109.5
C3—C2—N2 115.7 (2) C13—C14—H14B 109.5
C1—C2—N2 124.4 (2) H14A—C14—H14B 109.5
C2—C3—C4 120.06 (18) C13—C14—H14C 109.5
C2—C3—H3 120.0 H14A—C14—H14C 109.5
C4—C3—H3 120.0 H14B—C14—H14C 109.5
C3—C4—C5 122.90 (19) C16—C15—C20 121.9 (2)
C3—C4—N1 114.53 (17) C16—C15—N5 118.7 (2)
C5—C4—N1 122.53 (17) C20—C15—N5 119.4 (2)
C6—C5—C4 114.94 (17) C15—C16—C17 118.7 (2)
C6—C5—C7 120.57 (16) C15—C16—H16 120.7
C4—C5—C7 124.27 (17) C17—C16—H16 120.7
C1—C6—C5 123.20 (18) C16—C17—C18 119.8 (3)
C1—C6—H6 118.4 C16—C17—H17 120.1
C5—C6—H6 118.4 C18—C17—H17 120.1
C8—C7—C10 119.95 (16) C19—C18—C17 120.2 (3)
C8—C7—C5 118.54 (15) C19—C18—H18 119.9
C10—C7—C5 121.33 (15) C17—C18—H18 119.9
O7—C8—N3 117.64 (16) C20—C19—C18 120.8 (3)
O7—C8—C7 125.00 (16) C20—C19—H19 119.6
N3—C8—C7 117.34 (15) C18—C19—H19 119.6
O6—C9—N3 122.27 (17) C19—C20—C15 118.6 (3)
O6—C9—N4 121.96 (17) C19—C20—H20 120.7
N3—C9—N4 115.77 (17) C15—C20—H20 120.7
C9—N4—C10 125.86 (15) O1—N1—O2 123.6 (2)
C9—N4—H4A 115.2 (15) O1—N1—C4 118.06 (18)
C10—N4—H4A 118.9 (15) O2—N1—C4 118.25 (18)
C12—C11—H11A 109.5 O4—N2—O3 122.8 (2)
C12—C11—H11B 109.5 O4—N2—C2 120.0 (2)
H11A—C11—H11B 109.5 O3—N2—C2 117.2 (2)
C12—C11—H11C 109.5 C9—N3—C8 125.13 (16)
H11A—C11—H11C 109.5 C9—N3—H3A 116.8 (15)
H11B—C11—H11C 109.5 C8—N3—H3A 118.1 (15)
C11—C12—N5 112.2 (2) O5—C10—N4 117.47 (15)
C11—C12—H12A 109.2 O5—C10—C7 126.66 (16)
N5—C12—H12A 109.2 N4—C10—C7 115.85 (15)
C11—C12—H12B 109.2 C15—N5—C13 110.66 (19)
N5—C12—H12B 109.2 C15—N5—C12 113.4 (2)
H12A—C12—H12B 107.9 C13—N5—C12 113.49 (19)
C14—C13—N5 114.3 (3) C15—N5—H5A 110.8 (17)
C14—C13—H13A 108.7 C13—N5—H5A 105.5 (17)
N5—C13—H13A 108.7 C12—N5—H5A 102.4 (17)
C6—C1—C2—C3 1.4 (3) C17—C18—C19—C20 0.2 (4)
Cl1—C1—C2—C3 177.04 (16) C18—C19—C20—C15 −0.2 (4)
C6—C1—C2—N2 −176.22 (18) C16—C15—C20—C19 0.6 (4)
Cl1—C1—C2—N2 −0.6 (3) N5—C15—C20—C19 −178.9 (2)
C1—C2—C3—C4 −0.9 (3) C3—C4—N1—O1 −136.1 (2)
N2—C2—C3—C4 176.96 (17) C5—C4—N1—O1 41.9 (3)
C2—C3—C4—C5 −1.9 (3) C3—C4—N1—O2 40.2 (3)
C2—C3—C4—N1 176.06 (18) C5—C4—N1—O2 −141.9 (2)
C3—C4—C5—C6 3.8 (3) C3—C2—N2—O4 166.9 (2)
N1—C4—C5—C6 −173.95 (17) C1—C2—N2—O4 −15.4 (3)
C3—C4—C5—C7 −170.75 (18) C3—C2—N2—O3 −13.0 (3)
N1—C4—C5—C7 11.5 (3) C1—C2—N2—O3 164.7 (2)
C2—C1—C6—C5 0.8 (3) O6—C9—N3—C8 −179.2 (2)
Cl1—C1—C6—C5 −175.12 (16) N4—C9—N3—C8 0.4 (3)
C4—C5—C6—C1 −3.2 (3) O7—C8—N3—C9 178.2 (2)
C7—C5—C6—C1 171.53 (18) C7—C8—N3—C9 −0.2 (3)
C6—C5—C7—C8 −130.8 (2) C9—N4—C10—O5 −178.0 (2)
C4—C5—C7—C8 43.4 (3) C9—N4—C10—C7 3.3 (3)
C6—C5—C7—C10 44.3 (3) C8—C7—C10—O5 178.5 (2)
C4—C5—C7—C10 −141.4 (2) C5—C7—C10—O5 3.4 (3)
C10—C7—C8—O7 −176.7 (2) C8—C7—C10—N4 −3.0 (3)
C5—C7—C8—O7 −1.5 (3) C5—C7—C10—N4 −178.07 (17)
C10—C7—C8—N3 1.6 (3) C16—C15—N5—C13 110.6 (2)
C5—C7—C8—N3 176.84 (18) C20—C15—N5—C13 −69.9 (3)
O6—C9—N4—C10 177.5 (2) C16—C15—N5—C12 −120.5 (2)
N3—C9—N4—C10 −2.0 (3) C20—C15—N5—C12 59.0 (3)
C20—C15—C16—C17 −0.9 (3) C14—C13—N5—C15 −159.4 (3)
N5—C15—C16—C17 178.5 (2) C14—C13—N5—C12 71.8 (4)
C15—C16—C17—C18 0.9 (4) C11—C12—N5—C15 54.0 (3)
C16—C17—C18—C19 −0.5 (4) C11—C12—N5—C13 −178.6 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N4—H4A···O5i 0.83 (2) 2.06 (2) 2.892 (2) 175 (2)
N3—H3A···O7ii 0.83 (2) 1.96 (2) 2.794 (2) 180 (3)
N5—H5A···O6iii 0.87 (3) 1.82 (3) 2.677 (2) 168 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5583).

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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 datablock(s) global, I. DOI: 10.1107/S1600536813004352/lh5583sup1.cif

e-69-0o398-sup1.cif (30.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813004352/lh5583Isup2.hkl

e-69-0o398-Isup2.hkl (188KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813004352/lh5583Isup3.cml

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


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