Experimental. Crystal data. C 18 H 22 N 4 O 6 M r = Monoclinic, P2=n a = (5) Å b = (4) Å c = (5) Å = 104.

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organic compounds Acta Crystallographica Section E Structure Reports Online ISSN 1600-5368 Ethyl 5-((1E)-1-{(E)-2-[1-(4-ethoxycarbonyl-3-methyl-1,2-oxazol-5-yl)ethylidene]hydrazin-1-ylidene}ethyl)-3- methyl-1,2-oxazole-4-carboxylate Abdullah M. Asiri, a,b Abdulrahman O. Al-Youbi, a Hassan M. Faidallah, a Seik Weng Ng c,a and Edward R. T. Tiekink c * a Chemistry Department, Faculty of Science, King Abdulaziz University, PO Box 80203, Jeddah, Saudi Arabia, b The Center of Excellence for Advanced Materials Research, King Abdulaziz University, Jeddah, PO Box 80203, Saudi Arabia, and c Department of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia Correspondence e-mail: edward.tiekink@gmail.com Experimental Crystal data C 18 H 22 N 4 O 6 M r = 390.40 Monoclinic, P2=n a = 9.4509 (5) Å b = 8.5456 (4) Å c = 11.9859 (5) Å = 104.107 (5) Data collection Agilent SuperNova Dual diffractometer with Atlas detector Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.889, T max = 1.000 Refinement R[F 2 >2(F 2 )] = 0.049 wr(f 2 ) = 0.159 S = 0.87 2095 reflections V = 938.83 (8) Å 3 Z =2 Mo K radiation = 0.11 mm 1 T = 100 K 0.25 0.25 0.05 mm 4223 measured reflections 2095 independent reflections 1639 reflections with I > 2(I) R int = 0.023 129 parameters H-atom parameters constrained max = 0.37 e Å 3 min = 0.32 e Å 3 Received 7 August 2011; accepted 8 August 2011 Key indicators: single-crystal X-ray study; T = 100 K; mean (C C) = 0.003 Å; R factor = 0.049; wr factor = 0.159; data-to-parameter ratio = 16.2. The complete molecule of the title compound, C 18 H 22 N 4 O 6,is generated by the application of a twofold axis of symmetry. Twists are evident in the molecule, i.e. between each C N N group and the adjacent oxazole ring [dihedral angle = 46.08 (12) ] and between the latter and attached ester group [excluding the terminal methyl group; dihedral angle = 24.4 (7) ]. In the crystal, C HOand [3.5990 (11) Å] contacts connect molecules into supramolecular arrays in the ac plane. These stack along the b axis, being connected by weak [3.3903 (11) Å] interactions. Related literature For background to the biological activity of hydrazone compounds, see: Faid-Allah et al. (2011). Table 1 Hydrogen-bond geometry (Å, ). D HA D H HA DA D HA C9 H9cO2 i 0.98 2.46 3.356 (3) 152 Symmetry code: (i) x þ 1; y; z þ 1. Data collection: CrysAlis PRO (Agilent, 2010); 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). The authors thank King Abdulaziz University and the University of Malaya for supporting this study. Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5078). References Agilent (2010). CrysAlis PRO. Agilent Technologies, Yarnton, England. Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Faid-Allah, H. M., Khan, K. A. & Makki, M. S. I. (2011). J. Chin. Chem. Soc. 58, 191 198. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. Sheldrick, G. M. (2008). Acta Cryst. A64, 112 122. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920 925. Additional correspondence author, e-mail: aasiri2@kau.edu.sa. o2316 Asiri et al. doi:10.1107/s1600536811032004 Acta Cryst. (2011). E67, o2316

Acta Cryst. (2011). E67, o2316 [ doi:10.1107/s1600536811032004 ] Ethyl 5-((1E)-1-{(E)-2-[1-(4-ethoxycarbonyl-3-methyl-1,2-oxazol-5-yl)ethylidene]hydrazin-1- ylidene}ethyl)-3-methyl-1,2-oxazole-4-carboxylate A. M. Asiri, A. O. Al-Youbi, H. M. Faidallah, S. W. Ng and E. R. T. Tiekink Comment The study of the title compound (I) was motivated by the recent report of the significant anti-bacterial and anti-fungal activity exhibited hydrazone compounds (Faid-Allah et al., 2011). The full molecule of (I) is generated by the application of a 2-fold axis of symmetry. The configuration about the imine bond [1.280 (3) Å] is E. There are significant twists throughout the molecule. Firstly, the oxazole ring [r.m.s. deviation = 0.007 Å] is twisted away from the plane of the central C N N C group as seen in the value of the O1 C7 C8 N2 torsion angle of -43.3 (2). Further, the ester group lies out of the plane through the oxazole ring with the O2 C3 C6 C7 torsion angle being 160.5 (2). The oxazole-o atoms as well as the ester-ethyl groups are orientated towards the 2-fold axis while the carbonyl-o atoms are directed away from the axis. The terminal methyl group of the ester lies out of the plane of the remaining non-h atoms [the C3 O3 C2 C1 torsion angle = 159.33 (19) ]. Both C H O, Table 1, and π π interactions feature in the crystal packing. The C H O and π π contacts between oxazole rings [3.5990 (11) Å for symmetry operation 3/2 - x, y, 1.5 - z] combine to link molecules into supramolecular arrays in the ac plane, Fig. 2. These partially interdigitate with centrosymmetrically related layers along the b axis allowing for the formation of additional π π interactions [3.3903 (11) Å for symmetry operation 1 - x, 1 - y, 1 - z], Fig. 3. Experimental Ethyl 5-acetyl-2-methylthiazole-4-carboxylate (10 mmol) in C 2 H 5 OH (25 ml) was refluxed with hydrazine hydrate (12 mmol) for 1 h. The hydrazone which separated after concentration of the reaction mixture was filtered off, washed with C 2 H 5 OH, and recrystallized from C 2 H 5 OH; M.pt. 448 K. Refinement Carbon-bound H-atoms were placed in calculated positions [C H 0.98 to 0.99 Å, U iso (H) 1.2 to 1.5U eq (C)] and were included in the refinement in the riding model approximation. Figures Fig. 1. The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level. The molecule has crystallographic 2-fold symmetry and unlabelled atoms are generated by the symmetry operation 0.5 - x, y, 1.5 - z. sup-1

Fig. 2. Supramolecular array in the ac plane in (I) mediated by C H O and π π interactions shown as orange and purple dashed lines, respectively. Fig. 3. A view in projection down the a axis of the unit-cell contents of (I). The C H O and π π interactions are shown as orange and purple dashed lines, respectively. Ethyl 5-((1E)-1-{(E)-2-[1-(4-ethoxycarbonyl-3-methyl-1,2- oxazol-5-yl)ethylidene]hydrazin-1-ylidene}ethyl)-3- methyl-1,2-oxazole- 4-carboxylate Crystal data C 18 H 22 N 4 O 6 F(000) = 412 M r = 390.40 D x = 1.381 Mg m 3 Monoclinic, P2/n Mo Kα radiation, λ = 0.71073 Å Hall symbol: -P 2yac Cell parameters from 1742 reflections a = 9.4509 (5) Å θ = 2.4 29.3 b = 8.5456 (4) Å µ = 0.11 mm 1 c = 11.9859 (5) Å T = 100 K β = 104.107 (5) Plate, colourless V = 938.83 (8) Å 3 0.25 0.25 0.05 mm Z = 2 Data collection Agilent SuperNova Dual diffractometer with Atlas detector Radiation source: SuperNova (Mo) X-ray Source mirror R int = 0.023 2095 independent reflections 1639 reflections with I > 2σ(I) Detector resolution: 10.4041 pixels mm -1 θ max = 27.5, θ min = 2.4 ω scans Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) T min = 0.889, T max = 1.000 4223 measured reflections h = 11 11 k = 11 10 l = 14 15 Refinement Refinement on F 2 Primary atom site location: structure-invariant direct methods sup-2

Least-squares matrix: full R[F 2 > 2σ(F 2 )] = 0.049 wr(f 2 ) = 0.159 Secondary atom site location: difference Fourier map Hydrogen site location: inferred from neighbouring sites H-atom parameters constrained S = 0.87 w = 1/[σ 2 (F 2 o ) + (0.0921P) 2 + 1.4075P] where P = (F 2 o + 2F 2 c )/3 2095 reflections (Δ/σ) max < 0.001 129 parameters Δρ max = 0.37 e Å 3 0 restraints Δρ min = 0.32 e Å 3 Special details Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'s involving l.s. planes. Refinement. Refinement of F 2 against ALL reflections. The weighted R-factor wr and goodness of fit S are based on F 2, conventional R-factors R are based on F, with F set to zero for negative F 2. The threshold expression of F 2 > 2σ(F 2 ) is used only for calculating R- factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F 2 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 (Å 2 ) x y z U iso */U eq O1 0.54005 (15) 0.52943 (17) 0.63908 (12) 0.0176 (3) O2 0.67094 (17) 0.02949 (18) 0.57529 (14) 0.0248 (4) O3 0.51960 (17) 0.05289 (17) 0.69403 (12) 0.0202 (4) N1 0.67630 (19) 0.5276 (2) 0.60982 (14) 0.0186 (4) N2 0.32058 (18) 0.45172 (19) 0.74369 (14) 0.0162 (4) C1 0.4715 (3) 0.1526 (3) 0.8137 (2) 0.0309 (6) H1A 0.4662 0.2662 0.8231 0.046* H1B 0.3756 0.1062 0.8101 0.046* H1C 0.5434 0.1085 0.8792 0.046* C2 0.5158 (3) 0.1174 (3) 0.7054 (2) 0.0271 (5) H2A 0.6133 0.1623 0.7086 0.033* H2B 0.4450 0.1632 0.6387 0.033* C3 0.5997 (2) 0.1086 (3) 0.62488 (16) 0.0172 (4) C4 0.8420 (2) 0.3360 (3) 0.56290 (18) 0.0226 (5) H4A 0.8956 0.4309 0.5526 0.034* H4B 0.8161 0.2777 0.4904 0.034* H4C 0.9033 0.2705 0.6227 0.034* C5 0.7064 (2) 0.3801 (2) 0.59804 (16) 0.0161 (4) C6 0.5953 (2) 0.2805 (2) 0.62067 (15) 0.0150 (4) C7 0.4951 (2) 0.3805 (2) 0.64479 (16) 0.0148 (4) C8 0.3485 (2) 0.3616 (2) 0.66646 (16) 0.0153 (4) C9 0.2435 (2) 0.2483 (3) 0.59511 (18) 0.0201 (5) H9A 0.1556 0.3042 0.5542 0.030* sup-3

H9B 0.2170 0.1685 0.6451 0.030* H9C 0.2892 0.1980 0.5393 0.030* Atomic displacement parameters (Å 2 ) U 11 U 22 U 33 U 12 U 13 U 23 O1 0.0160 (7) 0.0156 (8) 0.0229 (7) 0.0016 (5) 0.0082 (6) 0.0009 (6) O2 0.0251 (9) 0.0214 (8) 0.0312 (8) 0.0041 (6) 0.0134 (7) 0.0046 (6) O3 0.0276 (8) 0.0123 (7) 0.0238 (8) 0.0014 (6) 0.0124 (6) 0.0017 (6) N1 0.0141 (8) 0.0240 (10) 0.0194 (8) 0.0022 (7) 0.0074 (7) 0.0010 (7) N2 0.0142 (9) 0.0152 (9) 0.0200 (8) 0.0015 (6) 0.0059 (7) 0.0020 (7) C1 0.0438 (15) 0.0198 (12) 0.0295 (12) 0.0039 (10) 0.0099 (11) 0.0041 (9) C2 0.0397 (14) 0.0120 (11) 0.0323 (12) 0.0001 (9) 0.0138 (10) 0.0017 (9) C3 0.0146 (10) 0.0192 (11) 0.0168 (9) 0.0006 (8) 0.0017 (8) 0.0006 (8) C4 0.0159 (10) 0.0304 (12) 0.0235 (10) 0.0016 (9) 0.0086 (8) 0.0012 (9) C5 0.0153 (9) 0.0201 (10) 0.0126 (9) 0.0000 (8) 0.0026 (7) 0.0014 (7) C6 0.0133 (9) 0.0182 (10) 0.0138 (9) 0.0004 (7) 0.0037 (7) 0.0010 (7) C7 0.0162 (10) 0.0143 (10) 0.0138 (9) 0.0010 (8) 0.0034 (7) 0.0014 (7) C8 0.0155 (10) 0.0129 (9) 0.0181 (9) 0.0004 (7) 0.0049 (7) 0.0030 (7) C9 0.0166 (10) 0.0226 (11) 0.0220 (10) 0.0030 (8) 0.0065 (8) 0.0034 (8) Geometric parameters (Å, ) O1 C7 1.349 (2) C2 H2B 0.9900 O1 N1 1.415 (2) C3 C6 1.470 (3) O2 C3 1.207 (2) C4 C5 1.492 (3) O3 C3 1.339 (2) C4 H4A 0.9800 O3 C2 1.462 (3) C4 H4B 0.9800 N1 C5 1.307 (3) C4 H4C 0.9800 N2 C8 1.280 (3) C5 C6 1.428 (3) N2 N2 i 1.379 (3) C6 C7 1.358 (3) C1 C2 1.489 (3) C7 C8 1.479 (3) C1 H1A 0.9800 C8 C9 1.496 (3) C1 H1B 0.9800 C9 H9A 0.9800 C1 H1C 0.9800 C9 H9B 0.9800 C2 H2A 0.9900 C9 H9C 0.9800 C7 O1 N1 108.63 (14) C5 C4 H4C 109.5 C3 O3 C2 116.20 (16) H4A C4 H4C 109.5 C5 N1 O1 105.79 (16) H4B C4 H4C 109.5 C8 N2 N2 i 117.04 (17) N1 C5 C6 111.43 (18) C2 C1 H1A 109.5 N1 C5 C4 119.89 (19) C2 C1 H1B 109.5 C6 C5 C4 128.67 (19) H1A C1 H1B 109.5 C7 C6 C5 104.37 (18) C2 C1 H1C 109.5 C7 C6 C3 129.58 (18) H1A C1 H1C 109.5 C5 C6 C3 125.88 (18) H1B C1 H1C 109.5 O1 C7 C6 109.77 (17) O3 C2 C1 107.50 (18) O1 C7 C8 115.58 (17) O3 C2 H2A 110.2 C6 C7 C8 134.47 (19) sup-4

C1 C2 H2A 110.2 N2 C8 C7 115.36 (17) O3 C2 H2B 110.2 N2 C8 C9 125.31 (18) C1 C2 H2B 110.2 C7 C8 C9 119.26 (17) H2A C2 H2B 108.5 C8 C9 H9A 109.5 O2 C3 O3 125.0 (2) C8 C9 H9B 109.5 O2 C3 C6 123.86 (19) H9A C9 H9B 109.5 O3 C3 C6 111.13 (17) C8 C9 H9C 109.5 C5 C4 H4A 109.5 H9A C9 H9C 109.5 C5 C4 H4B 109.5 H9B C9 H9C 109.5 H4A C4 H4B 109.5 C7 O1 N1 C5 0.7 (2) O3 C3 C6 C5 152.60 (18) C3 O3 C2 C1 159.33 (19) N1 O1 C7 C6 0.0 (2) C2 O3 C3 O2 2.3 (3) N1 O1 C7 C8 175.79 (15) C2 O3 C3 C6 179.88 (17) C5 C6 C7 O1 0.6 (2) O1 N1 C5 C6 1.1 (2) C3 C6 C7 O1 174.79 (18) O1 N1 C5 C4 177.90 (16) C5 C6 C7 C8 174.0 (2) N1 C5 C6 C7 1.1 (2) C3 C6 C7 C8 10.5 (4) C4 C5 C6 C7 177.79 (19) N2 i N2 C8 C7 172.11 (15) N1 C5 C6 C3 174.53 (18) N2 i N2 C8 C9 4.7 (3) C4 C5 C6 C3 6.6 (3) O1 C7 C8 N2 43.3 (2) O2 C3 C6 C7 160.5 (2) C6 C7 C8 N2 142.2 (2) O3 C3 C6 C7 21.9 (3) O1 C7 C8 C9 133.71 (19) O2 C3 C6 C5 25.0 (3) C6 C7 C8 C9 40.7 (3) Symmetry codes: (i) x+1/2, y, z+3/2. Hydrogen-bond geometry (Å, ) D H A D H H A D A D H A C9 H9c O2 ii 0.98 2.46 3.356 (3) 152 Symmetry codes: (ii) x+1, y, z+1. sup-5

Fig. 1 sup-6

Fig. 2 sup-7

Fig. 3 sup-8