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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jan 17;65(Pt 2):o325. doi: 10.1107/S160053680900124X

2-Benzoyl­amino-N-[5-(4-bromo­phen­yl)-1,3,4-thia­diazol-2-yl]ethanamide

Hui-Ming Huang a,b, Shi-Yuan Luo b, Shao-Hua Li b, Cheng-Mei Liu a,, Guo-Gang Tu b,*
PMCID: PMC2968191  PMID: 21581930

Abstract

In the structure of the title compound, C17H13BrN4O2S, the dihedral angle between the two benzene rings is 38.5 (1)°; the angle between the 4-bromo­benzene and thia­diazole rings is 1.3 (1)°. The conformations of the N—H and C=O bonds are anti with respect to each other. The structure displays inter­molecular N—H⋯O and C—H⋯O hydrogen bonding, with both interactions leading to inversion dimers.

Related literature

For 1,3,4-thia­diazole scaffold compounds and their biological activity, see: Tu et al. (2008). For the synthesis, see: Foroumadi et al. (1999); Levy & Palmer (1942); Song et al. (1992). For related structures, see: Gowda et al. (2008); Li, Huang et al. (2008); Li, Li et al. (2008).graphic file with name e-65-0o325-scheme1.jpg

Experimental

Crystal data

  • C17H13BrN4O2S

  • M r = 417.28

  • Triclinic, Inline graphic

  • a = 4.020 (4) Å

  • b = 13.706 (9) Å

  • c = 16.210 (5) Å

  • α = 113.334 (17)°

  • β = 94.018 (19)°

  • γ = 92.78 (2)°

  • V = 815.2 (10) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 2.67 mm−1

  • T = 298 (2) K

  • 0.54 × 0.17 × 0.04 mm

Data collection

  • Bruker X8 APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.591, T max = 0.914

  • 4633 measured reflections

  • 2592 independent reflections

  • 1097 reflections with I > 2σ(I)

  • R int = 0.082

Refinement

  • R[F 2 > 2σ(F 2)] = 0.109

  • wR(F 2) = 0.281

  • S = 0.82

  • 2592 reflections

  • 227 parameters

  • 6 restraints

  • H-atom parameters constrained

  • Δρmax = 1.67 e Å−3

  • Δρmin = −1.40 e Å−3

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: APEX2 (Bruker, 2004); software used to prepare material for publication: APEX2 (Bruker, 2004) and publCIF (Westrip, 2009).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680900124X/wn2304sup1.cif

e-65-0o325-sup1.cif (19.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680900124X/wn2304Isup2.hkl

e-65-0o325-Isup2.hkl (127.3KB, hkl)

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
C16—H16A⋯O2i 0.93 2.49 3.400 (5) 168
N2—H2A⋯O1ii 0.86 1.99 2.835 (5) 167

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

Acknowledgments

The work was supported by the Science and Technology Research Project of JiangXi Provincial Educational Department (No. GJJ09076), the Science and Technology Planning Project of JiangXi Provincial Health Department (No. 20082015) and the Natural Science Foundation of JiangXi Province, China.

supplementary crystallographic information

Comment

In our previous work, 1,3,4-thiadiazole scaffold compounds and their biological activity have been studied (Tu et al., 2008). In view of the importance of these organic materials, the title compound (Fig. 1) was synthesized (Foroumadi et al., 1999; Levy & Palmer 1942; Song et al., 1992) and its crystal structure is reported here.

In the structure of the title compound, C17H13BrN4O2S, the dihedral angle between the p-bromobenzene and thiadiazole rings is 1.3 (1)°; the angle between the two benzene rings is 38.5 (1)°. The conformations of the N—H and C═O bonds are anti with respect to each other. Bond lengths and angles are in normal ranges and comparable to those in related structures (Gowda et al., 2008; Li, Huang et al., 2008; Li, Li et al., 2008). In the crystal structure, molecules are linked through intermolecular C—H···O and N—H···O hydrogen bonds, forming a three-dimensional network (Table 1, Figure 2).

Experimental

N,N-Dicyclohexylcarbodiimide (5.7 mmol) was added to a cooled solution of N-benzoylglycine (5.6 mmol) and N-hydroxysuccinimide (5.6 mmol) in freshly distilled dioxane (30 ml). The reaction mixture was stirred overnight at room temperature. The insoluble material was filtered off and washed with cold dioxane. 2-Amino-5-(4-bromophenyl)-1,3,4-thiadiazole (5.5 mmol) was added to the filtrate and the reaction mixture was stirred for 48 h at room temperature. The solvent was removed under reduced pressure. The residue was dissolved in EtOAc and the insoluble material was filtered off. The filtrate was washed successively with saturated Na2CO3 solution (20 ml, x 3), water (20 ml, x 1), 0.1 M HCl (20 ml, x 3) and water (20 ml, x 1). The organic layer evaporated in vacuo, and the residue was recrystallized from methanol. Colorless block-shaped single crystals of the title compound suitable for X-ray diffraction analysis precipitated after several days.Yield: 37.0%; mp: 271–273°C.

Refinement

H atoms were positioned geometrically and refined using a riding model; Csp2—H = 0.93 Å, Csp3—H = 0.97 Å and N—H = 0.86 Å; Uĩso(H) = 1.2 Ueq(C,N). We made several attempts to obtain better quality data for this structure. However, due to poor crystal quality and possible disorder, the R and wR values are high. The maximum residual electron density occurs 1.23 Å from atom Br1, and the minimum residual electron density is located 1.29 Å from atom Br1.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound. Displacement ellipsoids are drawn at the 50% probability level. Hydrogen atoms are shown as spheres of arbitrary radius.

Fig. 2.

Fig. 2.

The crystal packing of the title compound, viewed along the a axis with hydrogen bonds drawn as dashed lines.

Crystal data

C17H13BrN4O2S Z = 2
Mr = 417.28 F(000) = 420.0
Triclinic, P1 Dx = 1.700 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 4.020 (4) Å Cell parameters from 1179 reflections
b = 13.706 (9) Å θ = 2.6–23.7°
c = 16.210 (5) Å µ = 2.67 mm1
α = 113.334 (17)° T = 298 K
β = 94.018 (19)° Block, colourless
γ = 92.78 (2)° 0.54 × 0.17 × 0.04 mm
V = 815.2 (10) Å3

Data collection

Bruker X8 APEXII diffractometer 2592 independent reflections
Radiation source: fine-focus sealed tube 1097 reflections with I > 2σ(I)
graphite Rint = 0.082
φ and ω scans θmax = 25.0°, θmin = 2.5°
Absorption correction: multi-scan (SADABS; Bruker, 2008) h = −4→4
Tmin = 0.591, Tmax = 0.914 k = −16→16
4633 measured reflections l = −19→19

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)] = 0.109 H-atom parameters constrained
wR(F2) = 0.281 w = 1/[σ2(Fo2) + (0.1951P)2] where P = (Fo2 + 2Fc2)/3
S = 0.82 (Δ/σ)max = 0.019
2592 reflections Δρmax = 1.67 e Å3
227 parameters Δρmin = −1.39 e Å3
6 restraints Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.022 (2)

Special details

Experimental. 1H-NMR (DMSO-d6): δ 4.24–4.25(d, J=5.08 Hz, 2H), 7.49–7.57 (m, 3H),7.73–7.75 (d, J=8.04 Hz, 2H), 7.89–7.91(t, J=3.60 Hz, 4H), 9.01 (s, 1H),12.91 (s, 1H). ESI-MS: m/z [M+H]+ 417.3.
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
Br1 0.19570 (14) 0.16142 (4) 0.64242 (3) 0.07526 (19)
S1 0.3284 (3) 0.41677 (8) 0.33059 (7) 0.0550 (4)
O1 0.2257 (8) 0.6333 (2) −0.00717 (17) 0.0636 (9)
O2 0.2253 (9) 0.5689 (2) 0.25867 (18) 0.0687 (8)
N1 0.2711 (9) 0.6635 (2) 0.1388 (2) 0.0551 (12)
H1A 0.2352 0.7034 0.1931 0.066*
N3 0.5949 (10) 0.2787 (3) 0.1998 (2) 0.0621 (13)
N4 0.5645 (10) 0.2351 (2) 0.2632 (2) 0.0597 (8)
N2 0.4834 (9) 0.4276 (2) 0.1728 (2) 0.0539 (8)
H2A 0.5726 0.3992 0.1229 0.065*
C4 −0.2078 (13) 0.9136 (3) 0.0368 (3) 0.0711 (18)
H4B −0.3108 0.9254 −0.0112 0.085*
C5 −0.0907 (12) 0.8176 (3) 0.0241 (3) 0.0610 (16)
H5A −0.1231 0.7628 −0.0332 0.073*
C10 0.4756 (11) 0.3703 (3) 0.2263 (3) 0.0512 (11)
C16 0.1797 (12) 0.3039 (3) 0.5556 (3) 0.0632 (17)
H16A 0.0838 0.3486 0.6061 0.076*
C15 0.2691 (13) 0.2067 (3) 0.5481 (3) 0.0603 (10)
C12 0.3711 (10) 0.2674 (3) 0.4098 (2) 0.0471 (9)
C14 0.4058 (11) 0.1370 (3) 0.4729 (3) 0.0598 (11)
H14A 0.4596 0.0701 0.4688 0.072*
C17 0.2354 (12) 0.3345 (3) 0.4857 (3) 0.0587 (11)
H17A 0.1807 0.4014 0.4900 0.070*
C8 0.4114 (12) 0.5638 (3) 0.1200 (3) 0.0560 (15)
H8A 0.6486 0.5723 0.1144 0.067*
H8B 0.3068 0.5116 0.0627 0.067*
C9 0.3647 (11) 0.5237 (3) 0.1913 (2) 0.0475 (10)
C11 0.4297 (11) 0.2963 (3) 0.3341 (2) 0.0483 (10)
C13 0.4598 (12) 0.1698 (3) 0.4041 (3) 0.0601 (16)
H13A 0.5571 0.1253 0.3537 0.072*
C7 0.1970 (11) 0.6938 (3) 0.0722 (3) 0.0521 (13)
C6 0.0730 (11) 0.7991 (3) 0.0926 (2) 0.0489 (14)
C2 −0.0154 (12) 0.9776 (3) 0.1919 (3) 0.0601 (16)
H2B 0.0074 1.0320 0.2494 0.072*
C3 −0.1698 (12) 0.9930 (3) 0.1230 (3) 0.0643 (17)
H3B −0.2533 1.0585 0.1332 0.077*
C1 0.1113 (12) 0.8805 (3) 0.1780 (3) 0.0555 (15)
H1B 0.2216 0.8701 0.2259 0.067*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.0941 (4) 0.0888 (3) 0.0604 (2) 0.0226 (3) 0.0361 (2) 0.04206 (19)
S1 0.0804 (8) 0.0441 (5) 0.0406 (5) 0.0193 (5) 0.0286 (5) 0.0118 (4)
O1 0.106 (2) 0.0501 (14) 0.0414 (6) 0.0279 (14) 0.0433 (10) 0.0174 (7)
O2 0.1043 (12) 0.0616 (16) 0.0469 (7) 0.0256 (13) 0.0439 (6) 0.0207 (9)
N1 0.082 (3) 0.0452 (17) 0.0435 (16) 0.0255 (16) 0.0332 (18) 0.0165 (13)
N3 0.099 (3) 0.0488 (17) 0.0448 (17) 0.0288 (18) 0.0270 (19) 0.0193 (13)
N4 0.1059 (15) 0.0386 (15) 0.0399 (8) 0.0252 (12) 0.0297 (7) 0.0154 (8)
N2 0.075 (2) 0.0474 (5) 0.0474 (5) 0.0157 (15) 0.0353 (16) 0.0212 (3)
C4 0.097 (4) 0.049 (2) 0.070 (3) 0.025 (2) 0.022 (3) 0.022 (2)
C5 0.080 (3) 0.042 (2) 0.053 (2) 0.012 (2) 0.009 (2) 0.0102 (18)
C10 0.073 (3) 0.0390 (7) 0.0442 (7) 0.0091 (19) 0.024 (2) 0.0156 (4)
C16 0.080 (3) 0.054 (2) 0.051 (2) 0.012 (2) 0.034 (2) 0.0102 (19)
C15 0.0825 (16) 0.0564 (19) 0.0442 (9) −0.0018 (12) 0.0194 (8) 0.0211 (8)
C12 0.0546 (15) 0.0498 (18) 0.0351 (9) 0.0036 (12) 0.0172 (7) 0.0131 (8)
C14 0.066 (2) 0.066 (2) 0.0600 (12) 0.0136 (14) 0.0282 (10) 0.0337 (10)
C17 0.078 (2) 0.050 (2) 0.0448 (11) 0.0131 (15) 0.0261 (10) 0.0109 (10)
C8 0.064 (3) 0.061 (2) 0.053 (2) 0.026 (2) 0.035 (2) 0.0269 (16)
C9 0.0644 (16) 0.041 (2) 0.0353 (8) 0.0082 (16) 0.0210 (7) 0.0104 (12)
C11 0.0753 (18) 0.0407 (18) 0.0336 (10) 0.0106 (14) 0.0223 (9) 0.0165 (9)
C13 0.094 (3) 0.042 (2) 0.046 (2) 0.010 (2) 0.030 (2) 0.0159 (16)
C7 0.071 (3) 0.047 (2) 0.0344 (7) 0.0104 (19) 0.0185 (14) 0.0105 (9)
C6 0.061 (3) 0.047 (2) 0.0339 (18) 0.0118 (19) 0.030 (2) 0.0067 (16)
C2 0.078 (3) 0.043 (2) 0.050 (2) 0.009 (2) 0.019 (2) 0.0062 (18)
C3 0.080 (3) 0.052 (2) 0.065 (3) 0.031 (2) 0.025 (3) 0.0211 (19)
C1 0.071 (3) 0.047 (2) 0.046 (2) 0.016 (2) 0.023 (2) 0.0120 (17)

Geometric parameters (Å, °)

Br1—C15 1.898 (5) C16—C17 1.382 (7)
S1—C10 1.714 (4) C16—H16A 0.9300
S1—C11 1.741 (5) C15—C14 1.387 (6)
O1—C7 1.242 (4) C12—C13 1.370 (6)
O2—C9 1.214 (5) C12—C17 1.380 (5)
N1—C7 1.323 (6) C12—C11 1.461 (6)
N1—C8 1.430 (5) C14—C13 1.383 (7)
N1—H1A 0.8600 C14—H14A 0.9300
N3—C10 1.285 (5) C17—H17A 0.9300
N3—N4 1.387 (6) C8—C9 1.483 (7)
N4—C11 1.299 (5) C8—H8A 0.9700
N2—C9 1.349 (5) C8—H8B 0.9700
N2—C10 1.381 (6) C13—H13A 0.9300
N2—H2A 0.8600 C7—C6 1.469 (6)
C4—C5 1.361 (7) C6—C1 1.383 (5)
C4—C3 1.382 (6) C2—C3 1.335 (7)
C4—H4B 0.9300 C2—C1 1.388 (6)
C5—C6 1.367 (7) C2—H2B 0.9300
C5—H5A 0.9300 C3—H3B 0.9300
C16—C15 1.359 (7) C1—H1B 0.9300
C10—S1—C11 86.0 (2) C16—C17—H17A 119.5
C7—N1—C8 119.6 (3) N1—C8—C9 112.3 (3)
C7—N1—H1A 120.2 N1—C8—H8A 109.1
C8—N1—H1A 120.2 C9—C8—H8A 109.1
C10—N3—N4 110.7 (4) N1—C8—H8B 109.1
C11—N4—N3 113.3 (3) C9—C8—H8B 109.1
C9—N2—C10 126.3 (3) H8A—C8—H8B 107.9
C9—N2—H2A 116.8 O2—C9—N2 121.9 (4)
C10—N2—H2A 116.8 O2—C9—C8 125.0 (4)
C5—C4—C3 118.3 (5) N2—C9—C8 113.1 (3)
C5—C4—H4B 120.9 N4—C11—C12 123.3 (4)
C3—C4—H4B 120.9 N4—C11—S1 113.4 (3)
C4—C5—C6 122.2 (4) C12—C11—S1 123.3 (3)
C4—C5—H5A 118.9 C12—C13—C14 120.4 (4)
C6—C5—H5A 118.9 C12—C13—H13A 119.8
N3—C10—N2 119.8 (4) C14—C13—H13A 119.8
N3—C10—S1 116.5 (4) O1—C7—N1 120.5 (4)
N2—C10—S1 123.6 (3) O1—C7—C6 120.0 (4)
C15—C16—C17 118.0 (4) N1—C7—C6 119.4 (3)
C15—C16—H16A 121.0 C5—C6—C1 118.3 (4)
C17—C16—H16A 121.0 C5—C6—C7 118.5 (3)
C16—C15—C14 122.6 (5) C1—C6—C7 123.2 (4)
C16—C15—Br1 119.4 (3) C3—C2—C1 120.2 (4)
C14—C15—Br1 118.0 (4) C3—C2—H2B 119.9
C13—C12—C17 119.7 (4) C1—C2—H2B 119.9
C13—C12—C11 117.6 (3) C2—C3—C4 121.2 (4)
C17—C12—C11 122.6 (4) C2—C3—H3B 119.4
C13—C14—C15 118.2 (4) C4—C3—H3B 119.4
C13—C14—H14A 120.9 C6—C1—C2 119.8 (4)
C15—C14—H14A 120.9 C6—C1—H1B 120.1
C12—C17—C16 121.0 (4) C2—C1—H1B 120.1
C12—C17—H17A 119.5
C10—N3—N4—C11 −1.0 (5) C13—C12—C11—N4 −0.9 (6)
C3—C4—C5—C6 −2.5 (8) C17—C12—C11—N4 178.3 (4)
N4—N3—C10—N2 179.7 (4) C13—C12—C11—S1 179.6 (3)
N4—N3—C10—S1 2.2 (5) C17—C12—C11—S1 −1.2 (6)
C9—N2—C10—N3 179.2 (4) C10—S1—C11—N4 1.5 (3)
C9—N2—C10—S1 −3.6 (6) C10—S1—C11—C12 −178.9 (4)
C11—S1—C10—N3 −2.2 (4) C17—C12—C13—C14 1.8 (6)
C11—S1—C10—N2 −179.5 (4) C11—C12—C13—C14 −179.0 (4)
C17—C16—C15—C14 −1.5 (7) C15—C14—C13—C12 −1.8 (7)
C17—C16—C15—Br1 −179.8 (3) C8—N1—C7—O1 5.2 (6)
C16—C15—C14—C13 1.7 (7) C8—N1—C7—C6 −176.1 (4)
Br1—C15—C14—C13 −179.9 (3) C4—C5—C6—C1 1.8 (7)
C13—C12—C17—C16 −1.6 (6) C4—C5—C6—C7 −178.7 (5)
C11—C12—C17—C16 179.2 (4) O1—C7—C6—C5 17.2 (7)
C15—C16—C17—C12 1.4 (7) N1—C7—C6—C5 −161.5 (4)
C7—N1—C8—C9 −159.0 (4) O1—C7—C6—C1 −163.3 (4)
C10—N2—C9—O2 −2.3 (6) N1—C7—C6—C1 18.0 (7)
C10—N2—C9—C8 −180.0 (4) C1—C2—C3—C4 0.1 (8)
N1—C8—C9—O2 −0.2 (6) C5—C4—C3—C2 1.6 (8)
N1—C8—C9—N2 177.4 (3) C5—C6—C1—C2 0.0 (7)
N3—N4—C11—C12 179.8 (4) C7—C6—C1—C2 −179.5 (4)
N3—N4—C11—S1 −0.6 (5) C3—C2—C1—C6 −0.9 (8)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C16—H16A···O2i 0.93 2.49 3.400 (5) 168
N2—H2A···O1ii 0.86 1.99 2.835 (5) 167

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WN2304).

References

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  11. Westrip, S. P. (2009). publCIF In preparation.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680900124X/wn2304sup1.cif

e-65-0o325-sup1.cif (19.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680900124X/wn2304Isup2.hkl

e-65-0o325-Isup2.hkl (127.3KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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