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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 19;68(Pt 6):o1768–o1769. doi: 10.1107/S1600536812020429

6-Methyl-1-({[(2E)-2-methyl-3-phenyl­prop-2-en-1-yl]­oxy}meth­yl)-1,2,3,4-tetra­hydro­quinazoline-2,4-dione

Nasser R El-Brollosy a,b,, Mohamed I Attia a, Ali A El-Emam a, Seik Weng Ng c,d, Edward R T Tiekink c,*
PMCID: PMC3379351  PMID: 22719549

Abstract

In the title compound, C20H20N2O3, the ten atoms comprising the quinazoline ring are essentially planar (r.m.s. deviation = 0.024 Å), and this plane is almost orthogonal to the terminal phenyl ring [dihedral angle = 82.87 (7)°]. The conformation about the ethyl­ene bond [1.335 (2) Å] is E and there is a significant twist between this residue and the adjacent phenyl ring [C—C—C— torsion angle = −48.4 (3)°]. The crystal structure features centrosymmetric dimeric units linked by pairs of N—H⋯O hydrogen bonds between the amide groups which lead to eight-membered {⋯HNCO}2 synthons. These are consolidated into a three-dimensional architecture by C—H⋯O, C—H⋯π and π–π inter­actions [centroid–centroid distances = 3.5087 (8) and 3.5645 (9) Å].

Related literature  

For background to non-nucleoside reverse transcriptase inhib­itors, see: Hopkins et al. (1996, 1999); El-Brollosy et al. (2008, 2009). For a related structure, see: El-Brollosy et al. (2012). For the synthesis, see: El-Brollosy (2007).graphic file with name e-68-o1768-scheme1.jpg

Experimental  

Crystal data  

  • C20H20N2O3

  • M r = 336.38

  • Monoclinic, Inline graphic

  • a = 16.2352 (8) Å

  • b = 13.6934 (6) Å

  • c = 7.8900 (4) Å

  • β = 102.606 (5)°

  • V = 1711.78 (14) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 100 K

  • 0.40 × 0.20 × 0.10 mm

Data collection  

  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) T min = 0.522, T max = 1.000

  • 13993 measured reflections

  • 3965 independent reflections

  • 3067 reflections with I > 2σ(I)

  • R int = 0.048

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.046

  • wR(F 2) = 0.129

  • S = 1.02

  • 3965 reflections

  • 232 parameters

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

  • Δρmax = 0.28 e Å−3

  • Δρmin = −0.25 e Å−3

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812020429/hg5224sup1.cif

e-68-o1768-sup1.cif (20.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020429/hg5224Isup2.hkl

e-68-o1768-Isup2.hkl (194.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812020429/hg5224Isup3.cml

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

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

Cg2 and Cg3 are the centroids of the C8–C8 and C15–C20 benzene rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1n⋯O2i 0.93 (2) 1.89 (2) 2.8180 (16) 172.9 (17)
C10—H10B⋯O1ii 0.99 2.49 3.3001 (18) 139
C11—H11B⋯O3iii 0.99 2.56 3.4462 (18) 150
C14—H14⋯Cg3iv 0.95 2.85 3.5574 (18) 132
C18—H18⋯Cg2iv 0.95 2.91 3.680 (2) 139

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

Acknowledgments

The financial support of the Deanship of Scientific Research and the Research Center of the College of Pharmacy, King Saud University is greatly appreciated. We also thank the Ministry of Higher Education (Malaysia) for funding structural studies through the High-Impact Research scheme (UM.C/HIR/MOHE/SC/12).

supplementary crystallographic information

Comment

In continuation of our interest in chemistry of non-nucleoside reverse transcriptase inhibitors (NNRTI's) (El-Brollosy et al., 2008; El-Brollosy et al., 2009), relevant to the treatment of human immunodeficiency virus (HIV) (Hopkins et al., 1996; Hopkins et al., 1999), we synthesized the title compound, 6-methyl-1-[((E)-2-methyl-3-phenylallyloxy)methyl]quinazoline-2,4(1H,3H)-dione (I), as a potential NNRTI (El-Brollosy, 2007). Herein, we describe the results of its crystal structure determination to complement the structure determination of the recently determined chloro analogue (El-Brollosy et al., 2012).

The 10 atoms comprising the quinazoline ring in (I), Fig. 1, are co-planar with a r.m.s. = 0.024 Å; the maximum deviations from their least-squares plane are 0.036 (1) Å for the C2 atom and -0.032 (1) Å for the N2 atom. The dihedral angle between the fused ring system and the terminal phenyl ring of 82.87 (7)° is consistent with an almost orthogonal relationship. The conformation about the ethylene bond [C12═C14 = 1.335 (2) Å] is E. The torsion angle between the ethylene and phenyl rings, i.e. C12—C14—C15—C16, of -48.4 (3)° indicates a significant twist about the C14—C15 bond. Overall, the molecule in (I) is significantly more twisted than that observed in the chloro analogue (El-Brollosy et al., 2012).

In the crystal structure, centrosymmetrically related molecules are connected via N—H···O hydrogen bonds between the amide groups (involving the carbonyl-O closest to the tertiary-N atom) which lead to eight-membered {···HNCO}2 synthons, Table 1. The dimeric aggregates are consolidated into a three-dimensional architecture by C—H···O and C—H···π interactions, Table 1, as well as by π—π contacts [ring centroid(N1,N2,C1–C3,C8)···centroid(N1,N2,C1–C3,C8)i = 3.5087 (8) Å and tilt angle = 0° and ring centroid(N1,N2,C1–C3,C8)···centroid(C3–C8)i = 3.5645 (9) Å and tilt angle = 1.85 (7)°, for symmetry operation i: 1 - x, 1 - y, -z). Globally, the crystal structure comprises alternating layers of quinazoline rings and 2-methyl-3-phenylallyloxy)methyl residues that stack along the a axis, Fig. 2.

Experimental

6-Methylquinazoline-2,4(1H,3H)dione (0.176 g, 1 mmol) was stirred in dry acetonitrile (15 ml) under nitrogen and N,O-bis(trimethylsilyl)acetamide (0.87 ml, 3.5 mmol) was added. After a clear solution was obtained (10 min), the mixture was cooled to 223 K and trimethylsilyl trifluoromethanesulfonate (0.18 ml, 1 mmol) was added followed by the drop-wise addition of bis[(E)-2-methyl-3-phenylallyloxy]methane (0.616 g, 2 mmol). The reaction mixture was stirred at room temperature for 5 h, after which the reaction was quenched by the addition of sat. aq. NaHCO3 solution (5 ml). The mixture was evaporated under reduced pressure and the residue was extracted with ether (3 × 50 ml). The combined ether fractions were collected, dried (MgSO4) and evaporated under reduced pressure. The product was purified on silica gel column chromatography, using 20% ether in petroleum ether (40–60°C), to afford the title compound as a white solid in 78% yield (0.262 g). Single crystals were achieved by recrystallization from its ethanol solution (El-Brollosy 2007).

Refinement

Carbon-bound H-atoms were placed in calculated positions [C—H = 0.95 to 0.99 Å, Uiso(H) = 1.2–1.5Ueq(C)] and were included in the refinement in the riding model approximation. The amino H-atom was refined freely.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

A view in projection down the c axis of the unit-cell contents for (I). The N—H···O, C—H···O, C—H···π and π—π interactions are shown as blue, orange, purple and brown dashed lines, respectively.

Crystal data

C20H20N2O3 F(000) = 712
Mr = 336.38 Dx = 1.305 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 4710 reflections
a = 16.2352 (8) Å θ = 2.6–27.5°
b = 13.6934 (6) Å µ = 0.09 mm1
c = 7.8900 (4) Å T = 100 K
β = 102.606 (5)° Prism, colourless
V = 1711.78 (14) Å3 0.40 × 0.20 × 0.10 mm
Z = 4

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 3965 independent reflections
Radiation source: SuperNova (Mo) X-ray Source 3067 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.048
Detector resolution: 10.4041 pixels mm-1 θmax = 27.6°, θmin = 2.6°
ω scan h = −21→20
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) k = −17→17
Tmin = 0.522, Tmax = 1.000 l = −10→8
13993 measured reflections

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)] = 0.046 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.129 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0571P)2 + 0.6389P] where P = (Fo2 + 2Fc2)/3
3965 reflections (Δ/σ)max < 0.001
232 parameters Δρmax = 0.28 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
O1 0.51870 (7) 0.31276 (7) 0.15509 (14) 0.0230 (3)
O2 0.55774 (7) 0.59676 (8) 0.45728 (13) 0.0209 (2)
O3 0.72545 (6) 0.70049 (7) 0.27942 (13) 0.0190 (2)
N1 0.53851 (8) 0.45651 (9) 0.30019 (16) 0.0180 (3)
H1n 0.5078 (12) 0.4335 (14) 0.379 (2) 0.030 (5)*
N2 0.60917 (7) 0.58944 (9) 0.21014 (16) 0.0162 (3)
C1 0.54810 (9) 0.39555 (10) 0.16689 (19) 0.0174 (3)
C2 0.56805 (9) 0.55065 (10) 0.32956 (18) 0.0169 (3)
C3 0.62603 (9) 0.53339 (11) 0.07198 (18) 0.0163 (3)
C4 0.67248 (9) 0.57169 (11) −0.04270 (19) 0.0186 (3)
H4 0.6932 0.6367 −0.0284 0.022*
C5 0.68806 (9) 0.51480 (11) −0.17644 (19) 0.0204 (3)
H5 0.7198 0.5418 −0.2530 0.024*
C6 0.65885 (9) 0.41867 (11) −0.20352 (19) 0.0202 (3)
C7 0.61195 (9) 0.38169 (11) −0.09098 (19) 0.0189 (3)
H7 0.5901 0.3172 −0.1078 0.023*
C8 0.59609 (9) 0.43757 (11) 0.04694 (18) 0.0169 (3)
C9 0.67858 (11) 0.35752 (12) −0.3488 (2) 0.0270 (4)
H9A 0.6299 0.3162 −0.3977 0.041*
H9B 0.7277 0.3162 −0.3034 0.041*
H9C 0.6909 0.4004 −0.4396 0.041*
C10 0.63668 (9) 0.69150 (10) 0.23222 (19) 0.0176 (3)
H10A 0.6155 0.7272 0.1222 0.021*
H10B 0.6117 0.7221 0.3230 0.021*
C11 0.76134 (9) 0.65578 (11) 0.44431 (19) 0.0201 (3)
H11A 0.7536 0.5841 0.4354 0.024*
H11B 0.7321 0.6802 0.5336 0.024*
C12 0.85380 (10) 0.67948 (11) 0.49682 (19) 0.0213 (3)
C13 0.87568 (10) 0.78634 (12) 0.5069 (2) 0.0258 (4)
H13A 0.9351 0.7945 0.5650 0.039*
H13B 0.8399 0.8206 0.5729 0.039*
H13C 0.8663 0.8135 0.3893 0.039*
C14 0.90837 (10) 0.60631 (12) 0.5433 (2) 0.0248 (4)
H14 0.8855 0.5422 0.5298 0.030*
C15 1.00037 (10) 0.61367 (12) 0.6133 (2) 0.0289 (4)
C16 1.03668 (12) 0.55823 (14) 0.7593 (3) 0.0376 (4)
H16 1.0020 0.5168 0.8105 0.045*
C17 1.12270 (13) 0.56292 (15) 0.8303 (3) 0.0468 (5)
H17 1.1464 0.5257 0.9307 0.056*
C18 1.17373 (12) 0.62174 (16) 0.7550 (3) 0.0481 (6)
H18 1.2326 0.6249 0.8038 0.058*
C19 1.13958 (12) 0.67605 (15) 0.6089 (3) 0.0430 (5)
H19 1.1749 0.7163 0.5570 0.052*
C20 1.05311 (11) 0.67162 (14) 0.5379 (3) 0.0342 (4)
H20 1.0299 0.7086 0.4368 0.041*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0252 (6) 0.0164 (5) 0.0286 (6) −0.0030 (4) 0.0084 (5) 0.0003 (4)
O2 0.0243 (6) 0.0206 (5) 0.0193 (6) −0.0032 (4) 0.0079 (4) −0.0011 (4)
O3 0.0172 (5) 0.0208 (5) 0.0190 (5) −0.0022 (4) 0.0041 (4) 0.0018 (4)
N1 0.0191 (6) 0.0181 (6) 0.0180 (6) −0.0017 (5) 0.0064 (5) 0.0020 (5)
N2 0.0163 (6) 0.0156 (6) 0.0169 (6) −0.0016 (5) 0.0039 (5) −0.0002 (5)
C1 0.0152 (7) 0.0171 (7) 0.0190 (7) 0.0009 (6) 0.0021 (5) 0.0021 (6)
C2 0.0142 (7) 0.0183 (7) 0.0176 (7) 0.0013 (6) 0.0023 (5) 0.0012 (6)
C3 0.0138 (7) 0.0174 (7) 0.0165 (7) 0.0019 (6) 0.0005 (5) 0.0006 (5)
C4 0.0176 (7) 0.0176 (7) 0.0201 (7) −0.0014 (6) 0.0029 (6) 0.0014 (6)
C5 0.0178 (7) 0.0246 (8) 0.0192 (7) 0.0016 (6) 0.0050 (6) 0.0035 (6)
C6 0.0191 (7) 0.0224 (8) 0.0185 (7) 0.0035 (6) 0.0031 (6) −0.0002 (6)
C7 0.0179 (7) 0.0175 (7) 0.0195 (7) 0.0010 (6) 0.0003 (6) 0.0008 (6)
C8 0.0136 (7) 0.0171 (7) 0.0191 (7) 0.0017 (6) 0.0018 (5) 0.0027 (6)
C9 0.0333 (9) 0.0248 (8) 0.0247 (8) 0.0034 (7) 0.0103 (7) −0.0021 (7)
C10 0.0179 (7) 0.0151 (7) 0.0198 (7) −0.0005 (6) 0.0040 (5) 0.0000 (5)
C11 0.0205 (8) 0.0209 (8) 0.0191 (7) 0.0008 (6) 0.0050 (6) 0.0018 (6)
C12 0.0212 (8) 0.0249 (8) 0.0180 (7) −0.0007 (6) 0.0046 (6) −0.0024 (6)
C13 0.0207 (8) 0.0237 (8) 0.0321 (9) −0.0002 (7) 0.0039 (6) −0.0027 (7)
C14 0.0236 (8) 0.0240 (8) 0.0258 (8) −0.0001 (7) 0.0031 (6) −0.0028 (6)
C15 0.0240 (9) 0.0244 (8) 0.0356 (10) 0.0048 (7) 0.0008 (7) −0.0077 (7)
C16 0.0331 (10) 0.0315 (10) 0.0426 (11) 0.0059 (8) −0.0043 (8) −0.0014 (8)
C17 0.0359 (11) 0.0375 (11) 0.0555 (13) 0.0104 (9) −0.0148 (9) −0.0033 (9)
C18 0.0217 (9) 0.0396 (11) 0.0736 (15) 0.0072 (9) −0.0104 (9) −0.0158 (11)
C19 0.0239 (9) 0.0392 (11) 0.0642 (14) −0.0002 (8) 0.0057 (9) −0.0135 (10)
C20 0.0250 (9) 0.0338 (10) 0.0419 (11) 0.0038 (8) 0.0034 (8) −0.0059 (8)

Geometric parameters (Å, º)

O1—C1 1.2257 (18) C10—H10A 0.9900
O2—C2 1.2311 (17) C10—H10B 0.9900
O3—C10 1.4130 (17) C11—C12 1.503 (2)
O3—C11 1.4409 (18) C11—H11A 0.9900
N1—C1 1.3780 (19) C11—H11B 0.9900
N1—C2 1.3773 (19) C12—C14 1.335 (2)
N1—H1n 0.93 (2) C12—C13 1.504 (2)
N2—C2 1.3749 (18) C13—H13A 0.9800
N2—C3 1.4081 (18) C13—H13B 0.9800
N2—C10 1.4659 (18) C13—H13C 0.9800
C1—C8 1.468 (2) C14—C15 1.479 (2)
C3—C8 1.398 (2) C14—H14 0.9500
C3—C4 1.400 (2) C15—C20 1.393 (3)
C4—C5 1.379 (2) C15—C16 1.397 (3)
C4—H4 0.9500 C16—C17 1.388 (3)
C5—C6 1.400 (2) C16—H16 0.9500
C5—H5 0.9500 C17—C18 1.379 (3)
C6—C7 1.386 (2) C17—H17 0.9500
C6—C9 1.509 (2) C18—C19 1.382 (3)
C7—C8 1.399 (2) C18—H18 0.9500
C7—H7 0.9500 C19—C20 1.395 (3)
C9—H9A 0.9800 C19—H19 0.9500
C9—H9B 0.9800 C20—H20 0.9500
C9—H9C 0.9800
C10—O3—C11 112.91 (11) O3—C10—H10B 109.1
C1—N1—C2 127.03 (13) N2—C10—H10B 109.1
C1—N1—H1n 118.0 (12) H10A—C10—H10B 107.9
C2—N1—H1n 114.9 (12) O3—C11—C12 109.88 (12)
C2—N2—C3 121.70 (12) O3—C11—H11A 109.7
C2—N2—C10 117.89 (12) C12—C11—H11A 109.7
C3—N2—C10 120.40 (11) O3—C11—H11B 109.7
O1—C1—N1 120.75 (13) C12—C11—H11B 109.7
O1—C1—C8 124.49 (13) H11A—C11—H11B 108.2
N1—C1—C8 114.76 (12) C14—C12—C13 125.52 (14)
O2—C2—N2 122.40 (13) C14—C12—C11 118.48 (14)
O2—C2—N1 120.88 (13) C13—C12—C11 115.78 (13)
N2—C2—N1 116.72 (12) C12—C13—H13A 109.5
C8—C3—C4 118.68 (13) C12—C13—H13B 109.5
C8—C3—N2 120.03 (13) H13A—C13—H13B 109.5
C4—C3—N2 121.29 (13) C12—C13—H13C 109.5
C5—C4—C3 119.85 (13) H13A—C13—H13C 109.5
C5—C4—H4 120.1 H13B—C13—H13C 109.5
C3—C4—H4 120.1 C12—C14—C15 127.40 (15)
C4—C5—C6 122.38 (14) C12—C14—H14 116.3
C4—C5—H5 118.8 C15—C14—H14 116.3
C6—C5—H5 118.8 C20—C15—C16 118.26 (16)
C7—C6—C5 117.47 (14) C20—C15—C14 122.97 (16)
C7—C6—C9 121.41 (14) C16—C15—C14 118.75 (17)
C5—C6—C9 121.12 (14) C17—C16—C15 120.9 (2)
C6—C7—C8 121.24 (14) C17—C16—H16 119.5
C6—C7—H7 119.4 C15—C16—H16 119.5
C8—C7—H7 119.4 C18—C17—C16 119.9 (2)
C3—C8—C7 120.38 (13) C18—C17—H17 120.0
C3—C8—C1 119.59 (13) C16—C17—H17 120.0
C7—C8—C1 120.04 (13) C17—C18—C19 120.27 (18)
C6—C9—H9A 109.5 C17—C18—H18 119.9
C6—C9—H9B 109.5 C19—C18—H18 119.9
H9A—C9—H9B 109.5 C18—C19—C20 119.8 (2)
C6—C9—H9C 109.5 C18—C19—H19 120.1
H9A—C9—H9C 109.5 C20—C19—H19 120.1
H9B—C9—H9C 109.5 C15—C20—C19 120.78 (18)
O3—C10—N2 112.40 (11) C15—C20—H20 119.6
O3—C10—H10A 109.1 C19—C20—H20 119.6
N2—C10—H10A 109.1
C2—N1—C1—O1 179.94 (14) C6—C7—C8—C1 −178.37 (13)
C2—N1—C1—C8 0.7 (2) O1—C1—C8—C3 179.38 (14)
C3—N2—C2—O2 175.15 (13) N1—C1—C8—C3 −1.44 (19)
C10—N2—C2—O2 −3.8 (2) O1—C1—C8—C7 −0.9 (2)
C3—N2—C2—N1 −4.7 (2) N1—C1—C8—C7 178.28 (13)
C10—N2—C2—N1 176.31 (12) C11—O3—C10—N2 −62.48 (15)
C1—N1—C2—O2 −177.56 (14) C2—N2—C10—O3 111.14 (14)
C1—N1—C2—N2 2.3 (2) C3—N2—C10—O3 −67.84 (16)
C2—N2—C3—C8 4.1 (2) C10—O3—C11—C12 −172.58 (12)
C10—N2—C3—C8 −176.95 (12) O3—C11—C12—C14 −128.83 (15)
C2—N2—C3—C4 −176.01 (13) O3—C11—C12—C13 56.34 (17)
C10—N2—C3—C4 2.9 (2) C13—C12—C14—C15 0.0 (3)
C8—C3—C4—C5 −0.3 (2) C11—C12—C14—C15 −174.30 (15)
N2—C3—C4—C5 179.85 (13) C12—C14—C15—C20 −48.4 (3)
C3—C4—C5—C6 0.1 (2) C12—C14—C15—C16 133.26 (19)
C4—C5—C6—C7 0.7 (2) C20—C15—C16—C17 1.9 (3)
C4—C5—C6—C9 −178.65 (14) C14—C15—C16—C17 −179.73 (17)
C5—C6—C7—C8 −1.5 (2) C15—C16—C17—C18 −1.0 (3)
C9—C6—C7—C8 177.92 (14) C16—C17—C18—C19 0.0 (3)
C4—C3—C8—C7 −0.4 (2) C17—C18—C19—C20 0.3 (3)
N2—C3—C8—C7 179.44 (13) C16—C15—C20—C19 −1.6 (3)
C4—C3—C8—C1 179.28 (13) C14—C15—C20—C19 −179.96 (16)
N2—C3—C8—C1 −0.8 (2) C18—C19—C20—C15 0.6 (3)
C6—C7—C8—C3 1.3 (2)

Hydrogen-bond geometry (Å, º)

Cg2 and Cg3 are the centroids of the C8–C8 and C15–C20 benzene rings, respectively.

D—H···A D—H H···A D···A D—H···A
N1—H1n···O2i 0.93 (2) 1.89 (2) 2.8180 (16) 172.9 (17)
C10—H10B···O1ii 0.99 2.49 3.3001 (18) 139
C11—H11B···O3iii 0.99 2.56 3.4462 (18) 150
C14—H14···Cg3iv 0.95 2.85 3.5574 (18) 132
C18—H18···Cg2iv 0.95 2.91 3.680 (2) 139

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5224).

References

  1. Agilent (2011). CrysAlis PRO Agilent Technologies, Yarnton, England.
  2. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. El-Brollosy, N. R. (2007). J. Chem. Res. pp. 358–361.
  4. El-Brollosy, N. R., Al-Deeb, O. A., El-Emam, A. A., Pedersen, E. B., La Colla, P., Collu, G., Sanna, G. & Loddo, R. (2009). Arch. Pharm. Chem. Life Sci. 342, 663–670. [DOI] [PubMed]
  5. El-Brollosy, N. R., Attia, M. I., El-Emam, A. A., Ng, S. W. & Tiekink, E. R. T. (2012). Acta Cryst. E68, o1770–o1771. [DOI] [PMC free article] [PubMed]
  6. El-Brollosy, N. R., Sorensen, E. R., Pedersen, E. B., Sanna, G., La Colla, P. & Loddo, R. (2008). Arch. Pharm. Chem. Life Sci. 341, 9–19. [DOI] [PubMed]
  7. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  8. Hopkins, A. L., Ren, J., Esnouf, R. M., Willcox, B. E., Jones, E. Y., Ross, C., Miyasaka, T., Walker, R. T., Tanaka, H., Stammers, D. K. & Stuart, D. I. (1996). J. Med. Chem. 39, 1589–1600. [DOI] [PubMed]
  9. Hopkins, A. L., Ren, J., Tanaka, H., Baba, M., Okamato, M., Stuart, D. I. & Stammers, D. K. (1999). J. Med. Chem. 42, 4500–4505. [DOI] [PubMed]
  10. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  11. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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/S1600536812020429/hg5224sup1.cif

e-68-o1768-sup1.cif (20.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812020429/hg5224Isup2.hkl

e-68-o1768-Isup2.hkl (194.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812020429/hg5224Isup3.cml

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


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