organic compounds
1-(5-Bromo-2-oxoindolin-3-ylidene)thiosemicarbazone
aEscola de Química e Alimentos, Universidade Federal do Rio Grande, Av. Itália km 08, Campus Carreiros, 96203-903 Rio Grande-RS, Brazil, bInstitut für Anorganische Chemie, Christian-Albrechts-Universität zu Kiel, Max-Eyth Strasse 2, D-24118 Kiel, Germany, and cDepartamento de Química, Universidade Federal de Sergipe, Av. Marechal Rondon s/n, Campus, 49100-000 São Cristóvão-SE, Brazil
*Correspondence e-mail: adriano@daad-alumni.de
The title molecule, C9H7BrN4OS, is essentially planar [r.m.s. deviation = 0.066 (2) Å], the maximum deviation from the mean plane through the non-H atoms being 0.190 (3) Å for the terminal amine N atom. In the crystal, molecules are linked through N—H⋯O and N—H⋯S interactions, generating infinite chains along the b-axis direction. In turn, the chains are stacked along the a axis via π–π interactions [centroid–centroid distance = 3.470 (2) Å] and further connected by N—H⋯Br interactions into a three-dimensional network. An intramolecular N—H⋯O hydrogen bond is also observed.
Related literature
For the pharmacological properties of isatin-thiosemicarbazone derivatives against cruzain, falcipain-2 and rhodesain, see: Chiyanzu et al. (2003). For the synthesis of 5-bromoisatin-3-thiosemicarbazone, see: Campaigne & Archer (1952). For the of 1-(5-bromo-2-oxoindolin-3-ylidene)thiosemicarbazide acetonitrile monosolvate, see: Pederzolli et al. (2011).
Experimental
Crystal data
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Data collection: X-AREA (Stoe & Cie, 2008); cell X-AREA; data reduction: X-RED32 (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
10.1107/S1600536813018564/lr2109sup1.cif
contains datablocks I, publication_text. DOI:Structure factors: contains datablock platon_shelxl. DOI: 10.1107/S1600536813018564/lr2109Isup2.hkl
Starting materials were commercially available and were used without further purification. The 5-bromoisatine-3-thiosemicarbazone synthesis was adapted from a procedure reported previously (Campaigne & Archer, 1952). A mixture of of 5-bromoisatin (8,83 mmol) and thiosemicarbazide (8,83 mmol) in ethanol (50 ml) in the presence of a catalytic amount of hydrochloric acid was refluxed for 6 h. After cooling and filtering, the title compound was obtained. Crystals suitable for X-ray diffraction of 5-bromoisatine-3-thiosemicarbazone were obtained unexpectedly from an unsuccessful reaction of SnCl2 dihydrate with the title compound in methanol and dichloromethane by the slow evaporation of the solvents. Elemental analysis(%): Calc. 36.01 C, 2.69 H, 18.67 N, 10.68 S; found 35.95 C, 2.25 H, 18.67 N, 10.60 S.
All non-hydrogen atoms were refined anisotropically. All C—H and N—H atoms were located in difference map but were positioned with idealized geometry and refined isotropically with Uiso(H) = 1.2 Ueq(C) using a riding model with C—H = 0.93 Å for aromatic and N—H = 0.86 Å for methyl H atoms. The terminal N—H atoms were located in difference map, their bond lengths were set to 0.86 Å and afterwards they were refined isotropically with Uiso(H) = 1.5 Ueq(N) using a riding model.
Data collection: X-AREA (Stoe & Cie, 2008); cell
X-AREA (Stoe & Cie, 2008); data reduction: X-RED32 (Stoe & Cie, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).Fig. 1. The molecular structure of the title compound with displacement ellipsoids drawn at the 40% probability level. | |
Fig. 2. Molecules of the title compound connected via N—H···S, N—H···O and N—H···Br interactions. H-interactions are indicated as dashed lines and the Figure is simplified for clarity. | |
Fig. 3. A view of the stacking along the crystallographic a-axis. The π–π-interactions are drawn as dashed lines.Symmetry codes are: (iv) x - 1,y,z; (v) x + 1,y,z. |
C9H7BrN4OS | Z = 4 |
Mr = 299.16 | F(000) = 592 |
Orthorhombic, P212121 | Dx = 1.794 Mg m−3 |
Hall symbol: P 2ac 2ab | Mo Kα radiation, λ = 0.71073 Å |
a = 4.0185 (2) Å | µ = 3.88 mm−1 |
b = 14.6418 (8) Å | T = 293 K |
c = 18.8276 (11) Å | Prism, yellow |
V = 1107.78 (10) Å3 | 0.10 × 0.06 × 0.04 mm |
Stoe IPDS-1 diffractometer | 2106 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube, Stoe IPDS-1 | Rint = 0.051 |
Graphite monochromator | θmax = 27.0°, θmin = 2.6° |
ϕ scans | h = −4→5 |
7791 measured reflections | k = −18→17 |
2405 independent reflections | l = −24→24 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.039 | w = 1/[σ2(Fo2) + (0.0516P)2 + 0.9296P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.091 | (Δ/σ)max < 0.001 |
S = 1.02 | Δρmax = 0.73 e Å−3 |
2405 reflections | Δρmin = −0.55 e Å−3 |
148 parameters | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.0123 (16) |
Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983), 951 Friedel pairs |
Secondary atom site location: difference Fourier map | Absolute structure parameter: −0.015 (13) |
C9H7BrN4OS | V = 1107.78 (10) Å3 |
Mr = 299.16 | Z = 4 |
Orthorhombic, P212121 | Mo Kα radiation |
a = 4.0185 (2) Å | µ = 3.88 mm−1 |
b = 14.6418 (8) Å | T = 293 K |
c = 18.8276 (11) Å | 0.10 × 0.06 × 0.04 mm |
Stoe IPDS-1 diffractometer | 2106 reflections with I > 2σ(I) |
7791 measured reflections | Rint = 0.051 |
2405 independent reflections |
R[F2 > 2σ(F2)] = 0.039 | H-atom parameters constrained |
wR(F2) = 0.091 | Δρmax = 0.73 e Å−3 |
S = 1.02 | Δρmin = −0.55 e Å−3 |
2405 reflections | Absolute structure: Flack (1983), 951 Friedel pairs |
148 parameters | Absolute structure parameter: −0.015 (13) |
0 restraints |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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. |
x | y | z | Uiso*/Ueq | ||
Br1 | 1.14379 (13) | 0.36317 (4) | 0.59001 (2) | 0.04209 (17) | |
S1 | −0.1204 (3) | 0.31338 (7) | 0.15460 (5) | 0.0298 (2) | |
O1 | 0.2574 (8) | 0.5699 (2) | 0.26587 (16) | 0.0352 (8) | |
N1 | 0.5769 (10) | 0.6107 (2) | 0.36442 (17) | 0.0271 (8) | |
H1 | 0.5788 | 0.6690 | 0.3590 | 0.033* | |
N2 | 0.3785 (9) | 0.3806 (2) | 0.32307 (15) | 0.0223 (6) | |
N3 | 0.2026 (9) | 0.3844 (2) | 0.26195 (17) | 0.0248 (7) | |
H3 | 0.1764 | 0.4359 | 0.2406 | 0.030* | |
N4 | 0.0979 (10) | 0.2311 (2) | 0.27236 (17) | 0.0285 (7) | |
H1N4 | 0.0154 | 0.1799 | 0.2562 | 0.029 (13)* | |
H2N4 | 0.1793 | 0.2242 | 0.3124 | 0.038 (15)* | |
C1 | 0.4265 (11) | 0.5512 (3) | 0.31935 (19) | 0.0254 (9) | |
C2 | 0.4870 (10) | 0.4577 (2) | 0.3483 (2) | 0.0209 (7) | |
C3 | 0.6801 (9) | 0.4700 (2) | 0.4126 (2) | 0.0213 (7) | |
C4 | 0.8021 (10) | 0.4087 (3) | 0.4623 (2) | 0.0253 (8) | |
H4 | 0.7701 | 0.3461 | 0.4574 | 0.030* | |
C5 | 0.9739 (11) | 0.4448 (3) | 0.5197 (2) | 0.0299 (9) | |
C6 | 1.0274 (11) | 0.5383 (3) | 0.5283 (2) | 0.0335 (10) | |
H6 | 1.1455 | 0.5597 | 0.5674 | 0.040* | |
C7 | 0.9031 (13) | 0.5993 (3) | 0.4782 (2) | 0.0344 (10) | |
H7 | 0.9363 | 0.6618 | 0.4832 | 0.041* | |
C8 | 0.7292 (10) | 0.5647 (3) | 0.4210 (2) | 0.0269 (9) | |
C9 | 0.0663 (9) | 0.3069 (3) | 0.2340 (2) | 0.0227 (8) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0320 (2) | 0.0652 (3) | 0.0290 (2) | −0.0030 (3) | −0.0044 (2) | 0.0148 (2) |
S1 | 0.0302 (5) | 0.0322 (5) | 0.0270 (4) | −0.0033 (5) | −0.0081 (5) | 0.0052 (4) |
O1 | 0.052 (2) | 0.0260 (14) | 0.0281 (14) | 0.0089 (13) | −0.0046 (13) | 0.0020 (12) |
N1 | 0.038 (2) | 0.0155 (15) | 0.0274 (16) | 0.0004 (13) | 0.0009 (15) | −0.0012 (11) |
N2 | 0.0221 (15) | 0.0232 (15) | 0.0218 (13) | 0.0011 (14) | −0.0005 (14) | −0.0003 (11) |
N3 | 0.030 (2) | 0.0213 (16) | 0.0228 (14) | 0.0008 (13) | −0.0016 (13) | 0.0024 (12) |
N4 | 0.035 (2) | 0.0228 (16) | 0.0272 (16) | −0.0010 (15) | −0.0076 (16) | 0.0050 (12) |
C1 | 0.030 (2) | 0.0227 (18) | 0.0233 (18) | 0.0025 (16) | 0.0038 (16) | 0.0031 (14) |
C2 | 0.0209 (18) | 0.0195 (17) | 0.0223 (17) | 0.0033 (14) | 0.0046 (14) | 0.0013 (14) |
C3 | 0.0202 (19) | 0.0214 (16) | 0.0224 (16) | −0.0034 (14) | 0.0063 (17) | −0.0001 (14) |
C4 | 0.020 (2) | 0.0313 (19) | 0.0241 (17) | −0.0021 (15) | 0.0031 (15) | 0.0055 (15) |
C5 | 0.021 (2) | 0.046 (2) | 0.0223 (18) | −0.0016 (17) | 0.0043 (15) | 0.0033 (17) |
C6 | 0.029 (2) | 0.045 (3) | 0.027 (2) | −0.0087 (19) | 0.0034 (17) | −0.0087 (18) |
C7 | 0.036 (3) | 0.036 (2) | 0.0306 (19) | −0.010 (2) | 0.010 (2) | −0.0104 (16) |
C8 | 0.030 (2) | 0.0275 (19) | 0.0236 (19) | −0.0019 (15) | 0.0086 (15) | −0.0031 (15) |
C9 | 0.018 (2) | 0.0256 (18) | 0.0248 (17) | −0.0018 (14) | 0.0051 (14) | 0.0014 (15) |
Br1—C5 | 1.910 (4) | N4—H2N4 | 0.8285 |
S1—C9 | 1.675 (4) | C1—C2 | 1.494 (5) |
O1—C1 | 1.245 (5) | C2—C3 | 1.449 (6) |
N1—C1 | 1.358 (5) | C3—C4 | 1.387 (5) |
N1—C8 | 1.400 (5) | C3—C8 | 1.409 (5) |
N1—H1 | 0.8598 | C4—C5 | 1.386 (6) |
N2—C2 | 1.299 (5) | C4—H4 | 0.9300 |
N2—N3 | 1.352 (4) | C5—C6 | 1.396 (6) |
N3—C9 | 1.367 (5) | C6—C7 | 1.392 (7) |
N3—H3 | 0.8600 | C6—H6 | 0.9300 |
N4—C9 | 1.330 (5) | C7—C8 | 1.381 (6) |
N4—H1N4 | 0.8746 | C7—H7 | 0.9300 |
C1—N1—C8 | 111.2 (3) | C5—C4—C3 | 117.1 (4) |
C1—N1—H1 | 124.5 | C5—C4—H4 | 121.4 |
C8—N1—H1 | 124.3 | C3—C4—H4 | 121.4 |
C2—N2—N3 | 116.8 (3) | C4—C5—C6 | 122.8 (4) |
N2—N3—C9 | 120.2 (3) | C4—C5—Br1 | 118.7 (3) |
N2—N3—H3 | 119.9 | C6—C5—Br1 | 118.5 (3) |
C9—N3—H3 | 119.9 | C7—C6—C5 | 119.7 (4) |
C9—N4—H1N4 | 119.3 | C7—C6—H6 | 120.2 |
C9—N4—H2N4 | 129.3 | C5—C6—H6 | 120.2 |
H1N4—N4—H2N4 | 111.2 | C8—C7—C6 | 118.4 (4) |
O1—C1—N1 | 127.3 (4) | C8—C7—H7 | 120.8 |
O1—C1—C2 | 125.9 (4) | C6—C7—H7 | 120.8 |
N1—C1—C2 | 106.7 (3) | C7—C8—N1 | 129.6 (4) |
N2—C2—C3 | 126.4 (3) | C7—C8—C3 | 121.3 (4) |
N2—C2—C1 | 127.4 (4) | N1—C8—C3 | 109.1 (3) |
C3—C2—C1 | 106.1 (3) | N4—C9—N3 | 116.4 (3) |
C4—C3—C8 | 120.7 (4) | N4—C9—S1 | 125.1 (3) |
C4—C3—C2 | 132.3 (3) | N3—C9—S1 | 118.4 (3) |
C8—C3—C2 | 106.9 (3) | ||
C2—N2—N3—C9 | −176.8 (4) | C3—C4—C5—C6 | −0.3 (6) |
C8—N1—C1—O1 | 176.5 (4) | C3—C4—C5—Br1 | 179.5 (3) |
C8—N1—C1—C2 | −0.5 (5) | C4—C5—C6—C7 | 0.5 (7) |
N3—N2—C2—C3 | −179.9 (4) | Br1—C5—C6—C7 | −179.3 (3) |
N3—N2—C2—C1 | 3.1 (6) | C5—C6—C7—C8 | 0.0 (7) |
O1—C1—C2—N2 | 0.6 (7) | C6—C7—C8—N1 | 179.1 (4) |
N1—C1—C2—N2 | 177.7 (4) | C6—C7—C8—C3 | −0.6 (6) |
O1—C1—C2—C3 | −176.9 (4) | C1—N1—C8—C7 | −179.1 (4) |
N1—C1—C2—C3 | 0.2 (4) | C1—N1—C8—C3 | 0.6 (5) |
N2—C2—C3—C4 | 0.9 (7) | C4—C3—C8—C7 | 0.8 (6) |
C1—C2—C3—C4 | 178.4 (4) | C2—C3—C8—C7 | 179.3 (4) |
N2—C2—C3—C8 | −177.4 (4) | C4—C3—C8—N1 | −178.9 (3) |
C1—C2—C3—C8 | 0.1 (4) | C2—C3—C8—N1 | −0.4 (4) |
C8—C3—C4—C5 | −0.3 (6) | N2—N3—C9—N4 | 4.4 (6) |
C2—C3—C4—C5 | −178.4 (4) | N2—N3—C9—S1 | −174.7 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···S1i | 0.86 | 2.82 | 3.507 (3) | 139 |
N3—H3···O1 | 0.86 | 2.04 | 2.726 (4) | 135 |
N4—H2N4···Br1ii | 0.83 | 2.91 | 3.665 (4) | 152 |
N4—H1N4···O1iii | 0.87 | 1.99 | 2.851 (4) | 167 |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) x−1/2, −y+1/2, −z+1; (iii) −x, y−1/2, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···S1i | 0.86 | 2.82 | 3.507 (3) | 139 |
N3—H3···O1 | 0.86 | 2.04 | 2.726 (4) | 135 |
N4—H2N4···Br1ii | 0.83 | 2.91 | 3.665 (4) | 152 |
N4—H1N4···O1iii | 0.87 | 1.99 | 2.851 (4) | 167 |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) x−1/2, −y+1/2, −z+1; (iii) −x, y−1/2, −z+1/2. |
Acknowledgements
We gratefully acknowledge financial support by the State of Schleswig–Holstein, Germany. We thank Professor Dr Wolfgang Bensch for access to his experimental facilities. We gratefully acknowledge financial support through the DECIT/SCTIE-MS-CNPq-FAPERGS-Pronem-# 11/2029–1 and PRONEX-CNPq-FAPERGS projects. KCTB thanks FAPEAM for the award of a scholarship and ABO acknowledges financial support through the FAPITEC/SE/FUNTEC/CNPq PPP 04/2011 program.
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Thiosemicarbazone derivatives have a wide range of biological properties. For example, isatin-based synthetic thiosemicarbazones show pharmacological activity against cruzain, falcipain-2 and rhodesain (Chiyanzu et al., 2003). As part of our study of thiosemicarbazone derivatives, we report herein the crystal structure of 5-bromoisatin-3-thiosemicarbazone (Campaigne & Archer, 1952). In the title compound, in which the molecular structure matches the asymmetric unit, the maximal deviation from the least squares plane through all non-hydrogen atoms amount to 0.1896 (32) Å for N4.The molecule shows an E conformation for the atoms about the N2—N3 bond (Fig. 1). The E conformation for the thiosemicarbazone fragment is also observed in the crystal structure of the 5-bromoisatin-3-thiosemicarbazone acetonitrile monosolvate (Pederzolli et al., 2011) and is related with the intramolecular N—H···O H-interaction (Table 1). The mean deviations from the least squares planes for the C1—C8/Br1/N1 and C9/N2—N4/S1 fragments amount to 0.0568 (26) Å for O1 and 0.0394 (27) Å for N3, respectively, and the dihedral angle between the two planes is 9.01 (12)°. The molecules are connected via centrosymmetric pairs of N—H···S and N—H···O interactions and additionally by N—H···Br interactions (Fig. 2 and Table 1) forming a three-dimensional hydrogen-bonded network, which stabilizes the crystal packing. Additionally, π–π-interactions are observed, with C···C distances = 3.396 (6) Å. The molecules are arranged in layers and are stacked into the crystallographic a-axis direction (Fig. 3).