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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):o1772–o1773. doi: 10.1107/S1600536812021393

3-(Adamantan-1-yl)-4-methyl-1-[(4-phenyl­piperazin-1-yl)meth­yl]-1H-1,2,4-triazole-5(4H)-thione dichloro­methane hemisolvate

Ali A El-Emam a,, Mohamed A Al-Omar a, Abdul-Malek S Al-Tamimi a, Seik Weng Ng b,c, Edward R T Tiekink b,*
PMCID: PMC3379353  PMID: 22719551

Abstract

The asymmetric unit of the title dichloro­methane hemisolvate, C24H33N5S·0.5CH2Cl2, comprises an adamantan­yl/triazole derivative and half a CH2Cl2 mol­ecule of crystallization; the latter is disordered about a twofold axis of symmetry. The piperazine ring has a chair conformation and the two N-bound substituents occupy equatorial positions. The piperazine residue is almost normal to the triazole ring [N—N—C—N torsion angle = −79.9 (3)°] so that to a first approximation, the mol­ecule has an L-shape. Linear supra­molecular chains parallel to [001] are formed via C—H⋯S inter­actions. Two such chains are linked into a double chain via C—H⋯Cl inter­actions involving the disordered CH2Cl2 mol­ecules of solvation.

Related literature  

For the diverse biological activities of adamantane derivatives, see: Al-Deeb et al. (2006); Al-Omar et al. (2010). For related adamantanyl structural studies, see: El-Emam et al. (2012a ,b ). For the preparation of one of the precursor mol­ecules, see: El-Emam & Ibrahim (1991).graphic file with name e-68-o1772-scheme1.jpg

Experimental  

Crystal data  

  • 2C24H33N5S·CH2Cl2

  • M r = 932.17

  • Orthorhombic, Inline graphic

  • a = 66.8490 (16) Å

  • b = 22.1076 (4) Å

  • c = 6.5109 (1) Å

  • V = 9622.3 (3) Å3

  • Z = 8

  • Cu Kα radiation

  • μ = 2.38 mm−1

  • T = 100 K

  • 0.30 × 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 = 0.752, T max = 1.000

  • 18884 measured reflections

  • 4509 independent reflections

  • 4437 reflections with I > 2σ(I)

  • R int = 0.025

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.045

  • wR(F 2) = 0.126

  • S = 1.09

  • 4509 reflections

  • 299 parameters

  • 19 restraints

  • H-atom parameters constrained

  • Δρmax = 0.41 e Å−3

  • Δρmin = −1.00 e Å−3

  • Absolute structure: Flack (1983), 1772 Friedel pairs

  • Flack parameter: −0.002 (17)

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/S1600536812021393/hg5226sup1.cif

e-68-o1772-sup1.cif (26.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812021393/hg5226Isup2.hkl

e-68-o1772-Isup2.hkl (221.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812021393/hg5226Isup3.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
C14—H14A⋯S1i 0.99 2.85 3.803 (3) 162
C16—H16A⋯Cl1 0.99 2.73 3.589 (4) 146

Symmetry code: (i) 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 the chemical and pharmacological properties of adamantane derivatives, motivated by their putative biological activities (Al-Deeb et al., 2006; Al-Omar et al., 2010), and as part of on-going structural studies (El-Emam et al., 2012a,b), we synthesized the title compound (I) as a potential chemotherapeutic agent. Herein, we describe the crystal and molecular structure of (I).

The asymmetric unit of (I), Fig. 1, comprises an adamantanyl/triazole derivative and half a CH2Cl2 molecule of crystallization. In the organic molecule, the piperazinyl ring has a chair conformation and the two N-bound substituents occupy equatorial positions. The piperazinyl residue is almost normal to the triazole ring with the N2—N3—C14—N4 torsion angle being -79.9 (3)°. To a first approximation, the molecule has an L-shape, as found recently in the 2-hydroxybenzylideneamino derivative (El-Emam et al., 2012a).

In the crystal packing, linear supramolecular chains parallel to [001] are formed via C—H···S interactions, Table 1. These are linked into a double chain via C—H···Cl interactions involving the disordered CH2Cl2 molecules of solvation, Fig. 2 and Table 1.

Experimental

A mixture of 3-(1-adamantyl)-4-methyl-4H-1,2,4-triazole-5-thiol (499 mg, 2 mmol), prepared according to the literature method (El-Emam & Ibrahim, 1991), 1-phenylpiperazine (325 mg, 2 mmol) and 37% formaldehyde solution (1 ml), in ethanol (8 ml), was heated under reflux for 15 min. when a clear solution was obtained. Stirring was continued for 12 h. at room temperature and the mixture was allowed to stand overnight. Cold water (5 ml) was slowly added and the mixture was stirred for 20 min. The precipitated crude product was filtered, washed with water, dried, and crystallized from ethanol to yield 635 mg (75%) of the title compound as colourless crystals. M.pt: 423–425 K. Single crystals suitable for X-ray analysis were obtained by slow evaporation of its CH2Cl2:EtOH solution held at room temperature (1:1; 5 ml). 1H NMR (CDCl3, 500.13 MHz): δ 1.77–1.84 (m, 6H, adamantane-H), 2.14 (s, 6H, adamantane-H), 2.27 (s, 3H, adamantane-H), 3.05 (s, 4H, piperazine-H), 3.27 (s, 4H, piperazine-H), 3.82 (s, 3H, CH3), 5.20 (s, 2H, CH2), 6.85–6.93 (m, 3H, Ar—H), 7.25–7.33 (m, 2H, Ar—H). 13C NMR (CDCl3, 125.76 MHz): δ 27.84, 33.97, 36.31, 39.02 (adamantane-C), 31.58 (CH3), 49.34, 50.40 (piperazine-C), 69.23 (CH2), 116.27, 119.86, 129.10, 151.33 (Ar—C), 156.31 (triazole C-5), 169.53 (C═S).

Refinement

The H-atoms were placed in calculated positions [and C—H = 0.95 to 1.00 Å, Uiso(H) = 1.2–1.5Ueq(C)] and were included in the refinement in the riding model approximation. A number of reflections, i.e. (8 0 0), (18 2 0), (6 2 0), (10 2 0) and (2 2 0), were omitted from the final cycles of refinement owing to poor agreement. The maximum and minimum residual electron density peaks of 0.41 and 1.00 e Å-3, respectively, were located 0.62 Å and 0.63 Å from the Cl1 and Cl2 atoms, respectively.

Figures

Fig. 1.

Fig. 1.

The molecular structures of the molecules comprising (I) showing the atom-labelling scheme and displacement ellipsoids at the 70% probability level. The CH2Cl2 molecule has 50% occupancy, being disordered over a twofold axis.

Fig. 2.

Fig. 2.

A view of the linear supramolecular double chain in (I). The C—H···S and C—H···Cl contacts are shown as orange and blue dashed lines, respectively. The CH2Cl2 molecule is disordered over two position; both orientations are displayed.

Crystal data

2C24H33N5S·CH2Cl2 F(000) = 3984
Mr = 932.17 Dx = 1.287 Mg m3
Orthorhombic, Fdd2 Cu Kα radiation, λ = 1.54184 Å
Hall symbol: F 2 -2d Cell parameters from 10015 reflections
a = 66.8490 (16) Å θ = 2.6–76.4°
b = 22.1076 (4) Å µ = 2.38 mm1
c = 6.5109 (1) Å T = 100 K
V = 9622.3 (3) Å3 Prism, colourless
Z = 8 0.30 × 0.20 × 0.10 mm

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 4509 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 4437 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.025
Detector resolution: 10.4041 pixels mm-1 θmax = 76.6°, θmin = 2.6°
ω scan h = −84→80
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) k = −25→27
Tmin = 0.752, Tmax = 1.000 l = −7→8
18884 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045 H-atom parameters constrained
wR(F2) = 0.126 w = 1/[σ2(Fo2) + (0.0825P)2 + 16.7617P] where P = (Fo2 + 2Fc2)/3
S = 1.09 (Δ/σ)max = 0.002
4509 reflections Δρmax = 0.41 e Å3
299 parameters Δρmin = −1.00 e Å3
19 restraints Absolute structure: Flack (1983), 1772 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.002 (17)

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 Occ. (<1)
S1 0.106131 (8) 0.22602 (2) 0.50061 (10) 0.02473 (15)
N1 0.09696 (3) 0.34338 (8) 0.4049 (3) 0.0198 (4)
N2 0.08323 (3) 0.33690 (8) 0.0966 (3) 0.0218 (4)
N3 0.08877 (3) 0.28044 (8) 0.1693 (3) 0.0219 (4)
N4 0.06533 (3) 0.20162 (8) 0.0489 (3) 0.0223 (4)
N5 0.02334 (3) 0.19119 (9) 0.1251 (3) 0.0256 (4)
C1 0.08658 (3) 0.44216 (9) 0.2235 (3) 0.0183 (4)
C2 0.07497 (4) 0.45691 (10) 0.0251 (4) 0.0256 (5)
H2A 0.0818 0.4383 −0.0939 0.031*
H2B 0.0613 0.4396 0.0337 0.031*
C3 0.07361 (4) 0.52562 (10) −0.0064 (5) 0.0262 (5)
H3 0.0661 0.5343 −0.1362 0.031*
C4 0.09476 (4) 0.55174 (10) −0.0222 (4) 0.0252 (5)
H4A 0.0941 0.5960 −0.0450 0.030*
H4B 0.1019 0.5333 −0.1400 0.030*
C5 0.10617 (4) 0.53843 (11) 0.1778 (4) 0.0252 (5)
H5 0.1199 0.5560 0.1685 0.030*
C6 0.09524 (5) 0.56653 (11) 0.3591 (5) 0.0356 (6)
H6A 0.0945 0.6110 0.3413 0.043*
H6B 0.1026 0.5579 0.4875 0.043*
C7 0.07398 (5) 0.54031 (11) 0.3735 (5) 0.0342 (6)
H7 0.0668 0.5591 0.4924 0.041*
C8 0.07510 (4) 0.47116 (10) 0.4044 (5) 0.0282 (5)
H8A 0.0614 0.4541 0.4118 0.034*
H8B 0.0820 0.4620 0.5352 0.034*
C9 0.10775 (3) 0.46982 (10) 0.2081 (4) 0.0220 (5)
H9A 0.1153 0.4610 0.3351 0.026*
H9B 0.1150 0.4516 0.0909 0.026*
C10 0.06261 (4) 0.55420 (11) 0.1747 (5) 0.0345 (6)
H10A 0.0489 0.5377 0.1834 0.041*
H10B 0.0617 0.5985 0.1550 0.041*
C11 0.08839 (3) 0.37444 (9) 0.2426 (4) 0.0199 (4)
C12 0.09709 (3) 0.28280 (10) 0.3552 (4) 0.0212 (4)
C13 0.10506 (4) 0.36501 (10) 0.5994 (4) 0.0245 (5)
H13A 0.1079 0.4084 0.5892 0.037*
H13B 0.1175 0.3432 0.6308 0.037*
H13C 0.0953 0.3580 0.7091 0.037*
C14 0.08542 (3) 0.22529 (9) 0.0446 (4) 0.0227 (5)
H14A 0.0890 0.2344 −0.0997 0.027*
H14B 0.0947 0.1934 0.0935 0.027*
C15 0.05794 (4) 0.18967 (13) 0.2540 (5) 0.0345 (6)
H15A 0.0564 0.2283 0.3293 0.041*
H15B 0.0677 0.1644 0.3292 0.041*
C16 0.03797 (4) 0.15741 (15) 0.2457 (6) 0.0427 (8)
H16A 0.0398 0.1168 0.1842 0.051*
H16B 0.0328 0.1519 0.3870 0.051*
C17 0.03096 (4) 0.20593 (11) −0.0794 (4) 0.0278 (5)
H17A 0.0212 0.2321 −0.1518 0.033*
H17B 0.0326 0.1683 −0.1602 0.033*
C18 0.05105 (4) 0.23845 (11) −0.0635 (4) 0.0261 (5)
H18A 0.0563 0.2468 −0.2030 0.031*
H18B 0.0492 0.2776 0.0078 0.031*
C19 0.00324 (4) 0.17111 (11) 0.1365 (4) 0.0281 (5)
C20 −0.01038 (4) 0.17995 (14) −0.0246 (5) 0.0366 (6)
H20 −0.0061 0.1985 −0.1485 0.044*
C21 −0.03030 (4) 0.16163 (14) −0.0037 (6) 0.0426 (7)
H21 −0.0393 0.1678 −0.1147 0.051*
C22 −0.03716 (4) 0.13510 (14) 0.1726 (6) 0.0404 (7)
H22 −0.0507 0.1227 0.1841 0.048*
C23 −0.02392 (4) 0.12670 (14) 0.3341 (6) 0.0421 (7)
H23 −0.0285 0.1087 0.4578 0.051*
C24 −0.00399 (4) 0.14421 (14) 0.3179 (5) 0.0365 (6)
H24 0.0048 0.1380 0.4304 0.044*
Cl1 0.02109 (2) 0.01531 (9) 0.0431 (3) 0.0562 (4) 0.50
Cl2 0.0020 (2) −0.0144 (4) −0.3345 (6) 0.143 (3) 0.50
C25 0.00259 (15) −0.0235 (4) −0.0659 (17) 0.073 (2) 0.50
H25A −0.0103 −0.0100 −0.0076 0.088* 0.50
H25B 0.0042 −0.0670 −0.0331 0.088* 0.50

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0326 (3) 0.0149 (2) 0.0267 (3) 0.0043 (2) 0.0009 (2) 0.0027 (2)
N1 0.0249 (9) 0.0129 (8) 0.0214 (10) 0.0011 (6) −0.0011 (7) −0.0014 (7)
N2 0.0278 (9) 0.0130 (8) 0.0248 (11) −0.0014 (7) 0.0005 (8) 0.0021 (8)
N3 0.0324 (10) 0.0115 (8) 0.0218 (10) −0.0020 (7) 0.0025 (8) 0.0002 (7)
N4 0.0244 (9) 0.0159 (8) 0.0266 (11) −0.0011 (7) 0.0011 (8) 0.0007 (8)
N5 0.0237 (9) 0.0280 (9) 0.0252 (11) 0.0024 (8) −0.0004 (8) 0.0046 (9)
C1 0.0202 (9) 0.0136 (9) 0.0212 (12) 0.0006 (7) 0.0027 (8) 0.0024 (8)
C2 0.0285 (11) 0.0162 (10) 0.0323 (14) 0.0006 (8) −0.0061 (10) 0.0003 (10)
C3 0.0293 (11) 0.0166 (10) 0.0328 (14) 0.0045 (8) −0.0026 (10) 0.0035 (10)
C4 0.0341 (12) 0.0160 (9) 0.0256 (13) 0.0007 (8) 0.0031 (10) 0.0045 (9)
C5 0.0311 (12) 0.0173 (10) 0.0274 (13) −0.0061 (8) −0.0017 (10) 0.0043 (9)
C6 0.0644 (18) 0.0135 (10) 0.0288 (15) −0.0043 (10) −0.0054 (13) −0.0001 (10)
C7 0.0535 (16) 0.0183 (10) 0.0308 (15) 0.0140 (10) 0.0160 (12) 0.0015 (10)
C8 0.0339 (12) 0.0184 (10) 0.0323 (15) 0.0062 (9) 0.0139 (10) 0.0059 (10)
C9 0.0211 (10) 0.0189 (10) 0.0259 (14) −0.0019 (7) 0.0023 (8) 0.0045 (9)
C10 0.0377 (13) 0.0223 (11) 0.0436 (16) 0.0123 (10) 0.0102 (12) 0.0069 (11)
C11 0.0197 (9) 0.0166 (9) 0.0234 (12) −0.0002 (7) 0.0010 (8) 0.0011 (9)
C12 0.0250 (10) 0.0136 (9) 0.0252 (12) −0.0006 (8) 0.0027 (9) −0.0018 (9)
C13 0.0323 (12) 0.0175 (10) 0.0239 (12) 0.0049 (8) −0.0056 (10) −0.0023 (9)
C14 0.0293 (11) 0.0151 (9) 0.0239 (13) −0.0028 (8) 0.0054 (9) −0.0037 (9)
C15 0.0240 (11) 0.0448 (14) 0.0348 (15) −0.0005 (10) −0.0018 (11) 0.0222 (13)
C16 0.0234 (11) 0.0544 (17) 0.0504 (19) −0.0021 (11) −0.0016 (12) 0.0336 (16)
C17 0.0292 (12) 0.0297 (12) 0.0244 (12) −0.0018 (9) −0.0028 (9) 0.0004 (10)
C18 0.0327 (12) 0.0231 (10) 0.0224 (12) −0.0025 (9) −0.0018 (9) 0.0044 (9)
C19 0.0243 (11) 0.0265 (11) 0.0335 (15) 0.0049 (9) 0.0024 (10) −0.0044 (10)
C20 0.0304 (12) 0.0439 (14) 0.0356 (17) 0.0019 (11) −0.0042 (11) 0.0003 (13)
C21 0.0277 (12) 0.0500 (16) 0.0500 (19) 0.0048 (11) −0.0068 (13) −0.0122 (15)
C22 0.0241 (12) 0.0406 (15) 0.057 (2) −0.0005 (10) 0.0028 (12) −0.0154 (14)
C23 0.0312 (13) 0.0454 (16) 0.0498 (19) −0.0028 (11) 0.0101 (13) 0.0008 (14)
C24 0.0279 (12) 0.0425 (15) 0.0391 (17) −0.0006 (10) 0.0028 (11) 0.0028 (13)
Cl1 0.0308 (7) 0.0813 (11) 0.0563 (11) 0.0133 (7) −0.0006 (6) −0.0114 (9)
Cl2 0.150 (5) 0.182 (8) 0.096 (2) −0.015 (6) 0.001 (3) −0.007 (3)
C25 0.074 (5) 0.059 (4) 0.086 (6) 0.008 (4) −0.001 (5) −0.005 (4)

Geometric parameters (Å, º)

S1—C12 1.684 (2) C8—H8A 0.9900
N1—C12 1.378 (3) C8—H8B 0.9900
N1—C11 1.384 (3) C9—H9A 0.9900
N1—C13 1.458 (3) C9—H9B 0.9900
N2—C11 1.308 (3) C10—H10A 0.9900
N2—N3 1.386 (2) C10—H10B 0.9900
N3—C12 1.333 (3) C13—H13A 0.9800
N3—C14 1.482 (3) C13—H13B 0.9800
N4—C14 1.442 (3) C13—H13C 0.9800
N4—C15 1.448 (3) C14—H14A 0.9900
N4—C18 1.453 (3) C14—H14B 0.9900
N5—C19 1.417 (3) C15—C16 1.515 (3)
N5—C16 1.460 (3) C15—H15A 0.9900
N5—C17 1.462 (3) C15—H15B 0.9900
C1—C11 1.507 (3) C16—H16A 0.9900
C1—C2 1.542 (3) C16—H16B 0.9900
C1—C9 1.545 (3) C17—C18 1.526 (3)
C1—C8 1.545 (3) C17—H17A 0.9900
C2—C3 1.536 (3) C17—H17B 0.9900
C2—H2A 0.9900 C18—H18A 0.9900
C2—H2B 0.9900 C18—H18B 0.9900
C3—C10 1.527 (4) C19—C20 1.403 (4)
C3—C4 1.531 (3) C19—C24 1.408 (4)
C3—H3 1.0000 C20—C21 1.398 (4)
C4—C5 1.538 (4) C20—H20 0.9500
C4—H4A 0.9900 C21—C22 1.368 (5)
C4—H4B 0.9900 C21—H21 0.9500
C5—C6 1.521 (4) C22—C23 1.386 (5)
C5—C9 1.533 (3) C22—H22 0.9500
C5—H5 1.0000 C23—C24 1.392 (4)
C6—C7 1.538 (4) C23—H23 0.9500
C6—H6A 0.9900 C24—H24 0.9500
C6—H6B 0.9900 Cl1—C25 1.664 (10)
C7—C10 1.532 (4) Cl2—C25 1.761 (12)
C7—C8 1.544 (3) C25—H25A 0.9900
C7—H7 1.0000 C25—H25B 0.9900
C12—N1—C11 107.82 (19) C3—C10—H10B 109.8
C12—N1—C13 121.3 (2) C7—C10—H10B 109.8
C11—N1—C13 130.84 (18) H10A—C10—H10B 108.3
C11—N2—N3 104.64 (19) N2—C11—N1 110.43 (18)
C12—N3—N2 112.72 (18) N2—C11—C1 123.3 (2)
C12—N3—C14 126.35 (19) N1—C11—C1 126.1 (2)
N2—N3—C14 120.92 (19) N3—C12—N1 104.39 (19)
C14—N4—C15 113.7 (2) N3—C12—S1 129.11 (17)
C14—N4—C18 113.51 (18) N1—C12—S1 126.51 (19)
C15—N4—C18 110.06 (19) N1—C13—H13A 109.5
C19—N5—C16 116.5 (2) N1—C13—H13B 109.5
C19—N5—C17 116.6 (2) H13A—C13—H13B 109.5
C16—N5—C17 111.7 (2) N1—C13—H13C 109.5
C11—C1—C2 108.64 (18) H13A—C13—H13C 109.5
C11—C1—C9 108.97 (17) H13B—C13—H13C 109.5
C2—C1—C9 108.83 (19) N4—C14—N3 115.42 (19)
C11—C1—C8 112.89 (18) N4—C14—H14A 108.4
C2—C1—C8 107.53 (19) N3—C14—H14A 108.4
C9—C1—C8 109.89 (19) N4—C14—H14B 108.4
C3—C2—C1 110.5 (2) N3—C14—H14B 108.4
C3—C2—H2A 109.5 H14A—C14—H14B 107.5
C1—C2—H2A 109.5 N4—C15—C16 110.7 (2)
C3—C2—H2B 109.5 N4—C15—H15A 109.5
C1—C2—H2B 109.5 C16—C15—H15A 109.5
H2A—C2—H2B 108.1 N4—C15—H15B 109.5
C10—C3—C4 109.9 (2) C16—C15—H15B 109.5
C10—C3—C2 109.5 (2) H15A—C15—H15B 108.1
C4—C3—C2 109.13 (18) N5—C16—C15 111.7 (2)
C10—C3—H3 109.4 N5—C16—H16A 109.3
C4—C3—H3 109.4 C15—C16—H16A 109.3
C2—C3—H3 109.4 N5—C16—H16B 109.3
C3—C4—C5 109.2 (2) C15—C16—H16B 109.3
C3—C4—H4A 109.8 H16A—C16—H16B 107.9
C5—C4—H4A 109.8 N5—C17—C18 110.5 (2)
C3—C4—H4B 109.8 N5—C17—H17A 109.6
C5—C4—H4B 109.8 C18—C17—H17A 109.6
H4A—C4—H4B 108.3 N5—C17—H17B 109.6
C6—C5—C9 109.7 (2) C18—C17—H17B 109.6
C6—C5—C4 109.9 (2) H17A—C17—H17B 108.1
C9—C5—C4 109.4 (2) N4—C18—C17 110.37 (19)
C6—C5—H5 109.3 N4—C18—H18A 109.6
C9—C5—H5 109.3 C17—C18—H18A 109.6
C4—C5—H5 109.3 N4—C18—H18B 109.6
C5—C6—C7 109.7 (2) C17—C18—H18B 109.6
C5—C6—H6A 109.7 H18A—C18—H18B 108.1
C7—C6—H6A 109.7 C20—C19—C24 117.6 (2)
C5—C6—H6B 109.7 C20—C19—N5 122.2 (3)
C7—C6—H6B 109.7 C24—C19—N5 120.1 (2)
H6A—C6—H6B 108.2 C21—C20—C19 120.3 (3)
C10—C7—C6 109.4 (2) C21—C20—H20 119.8
C10—C7—C8 109.4 (2) C19—C20—H20 119.8
C6—C7—C8 109.7 (2) C22—C21—C20 121.7 (3)
C10—C7—H7 109.5 C22—C21—H21 119.2
C6—C7—H7 109.5 C20—C21—H21 119.2
C8—C7—H7 109.5 C21—C22—C23 118.7 (3)
C7—C8—C1 109.6 (2) C21—C22—H22 120.7
C7—C8—H8A 109.8 C23—C22—H22 120.7
C1—C8—H8A 109.8 C22—C23—C24 121.1 (3)
C7—C8—H8B 109.8 C22—C23—H23 119.5
C1—C8—H8B 109.8 C24—C23—H23 119.5
H8A—C8—H8B 108.2 C23—C24—C19 120.6 (3)
C5—C9—C1 109.71 (18) C23—C24—H24 119.7
C5—C9—H9A 109.7 C19—C24—H24 119.7
C1—C9—H9A 109.7 Cl1—C25—Cl2 112.3 (8)
C5—C9—H9B 109.7 Cl1—C25—H25A 109.1
C1—C9—H9B 109.7 Cl2—C25—H25A 109.1
H9A—C9—H9B 108.2 Cl1—C25—H25B 109.1
C3—C10—C7 109.3 (2) Cl2—C25—H25B 109.1
C3—C10—H10A 109.8 H25A—C25—H25B 107.9
C7—C10—H10A 109.8
C11—N2—N3—C12 0.2 (2) C2—C1—C11—N1 −176.7 (2)
C11—N2—N3—C14 −179.6 (2) C9—C1—C11—N1 64.9 (3)
C11—C1—C2—C3 −177.29 (19) C8—C1—C11—N1 −57.5 (3)
C9—C1—C2—C3 −58.8 (2) N2—N3—C12—N1 −0.1 (2)
C8—C1—C2—C3 60.2 (2) N2—N3—C12—S1 −179.48 (17)
C1—C2—C3—C10 −60.5 (3) C14—N3—C12—S1 0.3 (3)
C1—C2—C3—C4 59.9 (3) C11—N1—C12—N3 0.0 (2)
C10—C3—C4—C5 59.7 (2) C13—N1—C12—N3 −179.56 (19)
C2—C3—C4—C5 −60.5 (3) C11—N1—C12—S1 179.40 (17)
C3—C4—C5—C6 −59.3 (2) C13—N1—C12—S1 −0.2 (3)
C3—C4—C5—C9 61.3 (2) C15—N4—C14—N3 −54.9 (3)
C9—C5—C6—C7 −60.9 (3) C18—N4—C14—N3 71.9 (3)
C4—C5—C6—C7 59.5 (3) C12—N3—C14—N4 100.3 (3)
C5—C6—C7—C10 −59.8 (3) N2—N3—C14—N4 −79.9 (3)
C5—C6—C7—C8 60.2 (3) C14—N4—C15—C16 −172.6 (2)
C10—C7—C8—C1 61.3 (3) C18—N4—C15—C16 58.8 (3)
C6—C7—C8—C1 −58.6 (3) C19—N5—C16—C15 −169.1 (3)
C11—C1—C8—C7 179.8 (2) C17—N5—C16—C15 53.3 (3)
C2—C1—C8—C7 −60.4 (3) N4—C15—C16—N5 −55.6 (3)
C9—C1—C8—C7 57.9 (3) C19—N5—C17—C18 168.7 (2)
C6—C5—C9—C1 60.0 (3) C16—N5—C17—C18 −53.8 (3)
C4—C5—C9—C1 −60.6 (3) C14—N4—C18—C17 171.5 (2)
C11—C1—C9—C5 177.2 (2) C15—N4—C18—C17 −59.8 (3)
C2—C1—C9—C5 58.9 (2) N5—C17—C18—N4 57.1 (3)
C8—C1—C9—C5 −58.6 (3) C16—N5—C19—C20 −152.3 (3)
C4—C3—C10—C7 −60.4 (3) C17—N5—C19—C20 −16.8 (3)
C2—C3—C10—C7 59.5 (3) C16—N5—C19—C24 31.2 (4)
C6—C7—C10—C3 59.9 (3) C17—N5—C19—C24 166.7 (2)
C8—C7—C10—C3 −60.2 (3) C24—C19—C20—C21 −0.9 (4)
N3—N2—C11—N1 −0.1 (2) N5—C19—C20—C21 −177.4 (2)
N3—N2—C11—C1 175.2 (2) C19—C20—C21—C22 0.4 (5)
C12—N1—C11—N2 0.1 (3) C20—C21—C22—C23 0.4 (5)
C12—N1—C11—C1 −175.1 (2) C21—C22—C23—C24 −0.6 (5)
C13—N1—C11—C1 4.4 (4) C22—C23—C24—C19 0.1 (5)
C2—C1—C11—N2 8.7 (3) C20—C19—C24—C23 0.6 (4)
C9—C1—C11—N2 −109.8 (2) N5—C19—C24—C23 177.2 (3)
C8—C1—C11—N2 127.9 (2)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C14—H14A···S1i 0.99 2.85 3.803 (3) 162
C16—H16A···Cl1 0.99 2.73 3.589 (4) 146

Symmetry code: (i) x, y, z−1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5226).

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 datablock(s) global, I. DOI: 10.1107/S1600536812021393/hg5226sup1.cif

e-68-o1772-sup1.cif (26.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812021393/hg5226Isup2.hkl

e-68-o1772-Isup2.hkl (221.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812021393/hg5226Isup3.cml

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


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