organic compounds
(Z)-1-[2-(Trifluoromethyl)benzylidene]thiosemicarbazide
aCollege of Sciences, Tianjin University of Science and Technology, Tianjin 300222, People's Republic of China
*Correspondence e-mail: jzl74@tust.edu.cn
In the 9H8F3N3S, all atoms except for two of the F atoms are located on a mirror plane. In the crystal, the molecules are connected by N—H⋯S hydrogen bonds, forming a molecular tape along the a axis.
of the title compound, CRelated literature
For general background to metal complexes with Shiff bases, see: Kahwa et al. (1986); Deng et al. (2005). For related structures, see: Guo et al. (2006); Jing et al. (2005); Santos et al. (2001); Yu et al. (2005).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 1999); cell SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
https://doi.org/10.1107/S1600536811047623/is2791sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536811047623/is2791Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S1600536811047623/is2791Isup3.cml
An anhydrous ethanol solution(50 mL) of thiosemicarbazide (0.91 g, 10 mmol) was added to an anhydrous ethanol solution(50 mL) of 2-(trifluoromethyl)benzaldehyde (1.74 g, 10 mmol) and the mixture was stirred at 350 K for 6 h under N2, whereupon a straw colorless solution appeared. The solvent was removed and the residue recrystallized from anhydrous ethanol. The product was isolated and then dried in vacuo to give pure (I) in 77% yield (Fig. 3). The colorless single crystals suitable for X-ray analysis were obtained by slow evaporation of an anhydrous ethanol solution of (I).
The N-bound H atoms were located in a difference Fourier map and their positions were refined freely with Uiso(H) = 1.2Ueq(N) [N—H = 0.82 (3)–0.93 (4) Å]. C-bound H atoms were included in calculated positions (C—H = 0.93 Å) and refined using the riding model approximation, with Uiso(H) = 1.2Ueq(C).
Metal complexes based on
have attracted much attention because they can be utilized as model compounds of active centres in various proteins and enzymes (Kahwa et al., 1986; Santos et al., 2001). As part of an investigation of the coordination properties of Shiff bases functioning as ligands (Yu et al., 2005; Deng et al., 2005; Jing, Fan et al., 2005; Guo, Sun et al., 2006), we report the synthesis and structure of the title compound, (I). In the molecular structure of the title compound (Fig. 1), the expected geometric parameters are observed. The molecules are associated via weak intermolecular N—H···S hydrogen-bonding interactions (Table 1) to form a supramolecular network as illustrated in Fig. 2.For general background to metal complexes with Shiff bases, see: Kahwa et al. (1986); Deng et al. (2005). For related structures, see: Guo et al. (2006); Jing et al. (2005); Santos et al. (2001); Yu et al. (2005).
Data collection: SMART (Bruker, 1999); cell
SAINT (Bruker, 1999); data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C9H8F3N3S | F(000) = 504 |
Mr = 247.24 | Dx = 1.497 Mg m−3 |
Orthorhombic, Pnma | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2n | Cell parameters from 2111 reflections |
a = 8.628 (2) Å | θ = 2.6–26.2° |
b = 6.9795 (17) Å | µ = 0.31 mm−1 |
c = 18.222 (4) Å | T = 294 K |
V = 1097.2 (5) Å3 | Block, colorless |
Z = 4 | 0.40 × 0.40 × 0.30 mm |
Bruker SMART APEX CCD area-detector diffractometer | 1228 independent reflections |
Radiation source: fine-focus sealed tube | 869 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.028 |
Detector resolution: 7.31 pixels mm-1 | θmax = 26.4°, θmin = 2.2° |
phi and ω scans | h = −10→7 |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | k = −7→8 |
Tmin = 0.886, Tmax = 0.912 | l = −22→22 |
5953 measured reflections |
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)] = 0.036 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.113 | w = 1/[σ2(Fo2) + (0.0497P)2 + 0.3737P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max = 0.001 |
1228 reflections | Δρmax = 0.19 e Å−3 |
101 parameters | Δρmin = −0.20 e Å−3 |
0 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: 0.0104 (19) |
C9H8F3N3S | V = 1097.2 (5) Å3 |
Mr = 247.24 | Z = 4 |
Orthorhombic, Pnma | Mo Kα radiation |
a = 8.628 (2) Å | µ = 0.31 mm−1 |
b = 6.9795 (17) Å | T = 294 K |
c = 18.222 (4) Å | 0.40 × 0.40 × 0.30 mm |
Bruker SMART APEX CCD area-detector diffractometer | 1228 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 869 reflections with I > 2σ(I) |
Tmin = 0.886, Tmax = 0.912 | Rint = 0.028 |
5953 measured reflections |
R[F2 > 2σ(F2)] = 0.036 | 0 restraints |
wR(F2) = 0.113 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.07 | Δρmax = 0.19 e Å−3 |
1228 reflections | Δρmin = −0.20 e Å−3 |
101 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.72882 (8) | 0.2500 | 1.28034 (4) | 0.0803 (4) | |
F1 | 0.0437 (2) | 0.2500 | 0.91939 (12) | 0.0999 (8) | |
F2 | 0.15033 (14) | 0.0964 (2) | 1.00795 (8) | 0.0891 (5) | |
N1 | 0.6005 (2) | 0.2500 | 1.07458 (11) | 0.0465 (6) | |
N2 | 0.5981 (2) | 0.2500 | 1.14995 (12) | 0.0519 (6) | |
H2A | 0.513 (4) | 0.2500 | 1.1704 (16) | 0.062* | |
N3 | 0.8620 (3) | 0.2500 | 1.14879 (15) | 0.0726 (9) | |
H3A | 0.862 (4) | 0.2500 | 1.098 (2) | 0.087* | |
H3B | 0.953 (5) | 0.2500 | 1.1704 (19) | 0.087* | |
C1 | 0.1665 (3) | 0.2500 | 0.96416 (18) | 0.0636 (8) | |
C2 | 0.3177 (3) | 0.2500 | 0.92383 (15) | 0.0490 (7) | |
C3 | 0.3171 (4) | 0.2500 | 0.84755 (17) | 0.0691 (9) | |
H3 | 0.2231 | 0.2500 | 0.8226 | 0.083* | |
C4 | 0.4530 (4) | 0.2500 | 0.80832 (18) | 0.0847 (11) | |
H4 | 0.4510 | 0.2500 | 0.7573 | 0.102* | |
C5 | 0.5928 (4) | 0.2500 | 0.84529 (17) | 0.0775 (10) | |
H5 | 0.6851 | 0.2500 | 0.8189 | 0.093* | |
C6 | 0.5970 (3) | 0.2500 | 0.92107 (16) | 0.0561 (8) | |
H6 | 0.6922 | 0.2500 | 0.9451 | 0.067* | |
C7 | 0.4604 (3) | 0.2500 | 0.96217 (14) | 0.0428 (6) | |
C8 | 0.4682 (3) | 0.2500 | 1.04285 (14) | 0.0442 (6) | |
H8 | 0.3777 | 0.2500 | 1.0706 | 0.053* | |
C9 | 0.7324 (3) | 0.2500 | 1.18753 (16) | 0.0538 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0329 (4) | 0.1575 (10) | 0.0504 (4) | 0.000 | −0.0050 (3) | 0.000 |
F1 | 0.0416 (10) | 0.161 (2) | 0.0973 (15) | 0.000 | −0.0225 (9) | 0.000 |
F2 | 0.0515 (7) | 0.1089 (12) | 0.1070 (11) | −0.0201 (7) | 0.0044 (7) | 0.0278 (10) |
N1 | 0.0349 (11) | 0.0577 (15) | 0.0469 (12) | 0.000 | 0.0003 (9) | 0.000 |
N2 | 0.0282 (11) | 0.0807 (18) | 0.0468 (12) | 0.000 | 0.0005 (9) | 0.000 |
N3 | 0.0300 (11) | 0.132 (3) | 0.0555 (14) | 0.000 | −0.0005 (11) | 0.000 |
C1 | 0.0383 (14) | 0.082 (2) | 0.071 (2) | 0.000 | −0.0100 (13) | 0.000 |
C2 | 0.0419 (13) | 0.0487 (16) | 0.0565 (15) | 0.000 | −0.0049 (12) | 0.000 |
C3 | 0.0595 (18) | 0.091 (3) | 0.0566 (17) | 0.000 | −0.0154 (14) | 0.000 |
C4 | 0.074 (2) | 0.129 (3) | 0.0511 (17) | 0.000 | −0.0017 (17) | 0.000 |
C5 | 0.062 (2) | 0.113 (3) | 0.0578 (18) | 0.000 | 0.0124 (15) | 0.000 |
C6 | 0.0410 (14) | 0.069 (2) | 0.0587 (16) | 0.000 | 0.0015 (12) | 0.000 |
C7 | 0.0381 (13) | 0.0409 (15) | 0.0495 (14) | 0.000 | −0.0003 (11) | 0.000 |
C8 | 0.0305 (12) | 0.0507 (16) | 0.0513 (14) | 0.000 | 0.0019 (10) | 0.000 |
C9 | 0.0321 (12) | 0.074 (2) | 0.0554 (15) | 0.000 | −0.0012 (11) | 0.000 |
S1—C9 | 1.691 (3) | C2—C3 | 1.390 (4) |
F1—C1 | 1.338 (3) | C2—C7 | 1.416 (3) |
F2—C1 | 1.343 (2) | C3—C4 | 1.373 (5) |
N1—C8 | 1.279 (3) | C3—H3 | 0.9300 |
N1—N2 | 1.374 (3) | C4—C5 | 1.381 (5) |
N2—C9 | 1.346 (3) | C4—H4 | 0.9300 |
N2—H2A | 0.82 (3) | C5—C6 | 1.381 (4) |
N3—C9 | 1.322 (3) | C5—H5 | 0.9300 |
N3—H3A | 0.93 (4) | C6—C7 | 1.397 (4) |
N3—H3B | 0.88 (4) | C6—H6 | 0.9300 |
C1—F2i | 1.343 (2) | C7—C8 | 1.472 (3) |
C1—C2 | 1.497 (4) | C8—H8 | 0.9300 |
C8—N1—N2 | 116.0 (2) | C3—C4—C5 | 119.4 (3) |
C9—N2—N1 | 119.7 (2) | C3—C4—H4 | 120.3 |
C9—N2—H2A | 122 (2) | C5—C4—H4 | 120.3 |
N1—N2—H2A | 118 (2) | C6—C5—C4 | 120.7 (3) |
C9—N3—H3A | 122 (2) | C6—C5—H5 | 119.7 |
C9—N3—H3B | 121 (2) | C4—C5—H5 | 119.7 |
H3A—N3—H3B | 117 (3) | C5—C6—C7 | 120.9 (3) |
F1—C1—F2i | 106.24 (16) | C5—C6—H6 | 119.5 |
F1—C1—F2 | 106.24 (16) | C7—C6—H6 | 119.5 |
F2i—C1—F2 | 105.8 (3) | C6—C7—C2 | 118.0 (2) |
F1—C1—C2 | 113.0 (3) | C6—C7—C8 | 119.8 (2) |
F2i—C1—C2 | 112.47 (15) | C2—C7—C8 | 122.2 (2) |
F2—C1—C2 | 112.47 (15) | N1—C8—C7 | 119.5 (2) |
C3—C2—C7 | 119.8 (3) | N1—C8—H8 | 120.3 |
C3—C2—C1 | 119.2 (3) | C7—C8—H8 | 120.3 |
C7—C2—C1 | 121.0 (2) | N3—C9—N2 | 117.1 (2) |
C4—C3—C2 | 121.2 (3) | N3—C9—S1 | 123.3 (2) |
C4—C3—H3 | 119.4 | N2—C9—S1 | 119.5 (2) |
C2—C3—H3 | 119.4 | ||
C8—N1—N2—C9 | 180.000 (1) | C5—C6—C7—C2 | 0.000 (2) |
F1—C1—C2—C3 | 0.000 (2) | C5—C6—C7—C8 | 180.000 (1) |
F2i—C1—C2—C3 | −120.30 (18) | C3—C2—C7—C6 | 0.000 (2) |
F2—C1—C2—C3 | 120.30 (18) | C1—C2—C7—C6 | 180.000 (1) |
F1—C1—C2—C7 | 180.000 (1) | C3—C2—C7—C8 | 180.000 (1) |
F2i—C1—C2—C7 | 59.70 (18) | C1—C2—C7—C8 | 0.000 (1) |
F2—C1—C2—C7 | −59.70 (18) | N2—N1—C8—C7 | 180.000 (1) |
C7—C2—C3—C4 | 0.000 (2) | C6—C7—C8—N1 | 0.000 (1) |
C1—C2—C3—C4 | 180.000 (1) | C2—C7—C8—N1 | 180.000 (1) |
C2—C3—C4—C5 | 0.000 (2) | N1—N2—C9—N3 | 0.000 (2) |
C3—C4—C5—C6 | 0.000 (2) | N1—N2—C9—S1 | 180.0 |
C4—C5—C6—C7 | 0.000 (2) |
Symmetry code: (i) x, −y+1/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3B···S1ii | 0.88 (4) | 2.54 (4) | 3.418 (3) | 174 (3) |
N2—H2A···S1iii | 0.82 (3) | 2.61 (3) | 3.430 (2) | 173 (3) |
Symmetry codes: (ii) x+1/2, y, −z+5/2; (iii) x−1/2, y, −z+5/2. |
Experimental details
Crystal data | |
Chemical formula | C9H8F3N3S |
Mr | 247.24 |
Crystal system, space group | Orthorhombic, Pnma |
Temperature (K) | 294 |
a, b, c (Å) | 8.628 (2), 6.9795 (17), 18.222 (4) |
V (Å3) | 1097.2 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.31 |
Crystal size (mm) | 0.40 × 0.40 × 0.30 |
Data collection | |
Diffractometer | Bruker SMART APEX CCD area-detector |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.886, 0.912 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5953, 1228, 869 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.626 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.036, 0.113, 1.07 |
No. of reflections | 1228 |
No. of parameters | 101 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.19, −0.20 |
Computer programs: SMART (Bruker, 1999), SAINT (Bruker, 1999), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N3—H3B···S1i | 0.88 (4) | 2.54 (4) | 3.418 (3) | 174 (3) |
N2—H2A···S1ii | 0.82 (3) | 2.61 (3) | 3.430 (2) | 173 (3) |
Symmetry codes: (i) x+1/2, y, −z+5/2; (ii) x−1/2, y, −z+5/2. |
Acknowledgements
This work was supported by the Tianjn University of Science and Technology Research Fund (No. 20090216).
References
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Metal complexes based on Schiff bases have attracted much attention because they can be utilized as model compounds of active centres in various proteins and enzymes (Kahwa et al., 1986; Santos et al., 2001). As part of an investigation of the coordination properties of Shiff bases functioning as ligands (Yu et al., 2005; Deng et al., 2005; Jing, Fan et al., 2005; Guo, Sun et al., 2006), we report the synthesis and structure of the title compound, (I). In the molecular structure of the title compound (Fig. 1), the expected geometric parameters are observed. The molecules are associated via weak intermolecular N—H···S hydrogen-bonding interactions (Table 1) to form a supramolecular network as illustrated in Fig. 2.