supplementary materials


lh5136 scheme

Acta Cryst. (2010). E66, o2685    [ doi:10.1107/S1600536810038389 ]

1-(3,4-Dimethylbenzylidene)-4-ethylthiosemicarbazide

Y.-F. Li and F.-Y. Meng

Abstract top

The title compound, C12H17N3S, was prepared by the reaction of 4-ethylthiosemicarbazide and 3,4-dimethylbenzaldehyde. The dihedral angle between the thiourea unit and the benzene ring is 7.09 (8)°. In the crystal, inversion dimers linked by pairs of N-H...S hydrogen bonds occur.

Comment top

Schiff-bases have attracted attention because they can be utilized as effective ligands in coordination chemistry (Casas et al., 2000). They are important intermediates which have been reported to form chiral coordination compounds with many interesting properties (Habermehl et al., 2006). As part of our research on new Schiff-base compounds we synthesized the title compound (I), and have determined its crystal structure. The molecular structure is shown in Fig. 1. The dihedral angle between the benzene ring and the thiourea unit is 7.09 (8)°. The bond lengths and angles agree with those observed in 4-Ethyl-1-(4-methylbenzylidene)thiosemicarbazide (Li & Jian, 2010). In the crystal structure, centrosymmetric dimers are formed by pairs of intermolecular N—H···S hydrogen bonds.

Related literature top

For applications of Schiff base compounds, see: Casas et al. (2000); Habermehl et al. (2006). For the structure of 4-ethyl-1-(4-methylbenzylidene)thiosemicarbazide, see: Li & Jian (2010).

Experimental top

A mixture of the 4-ethylthiosemicarbazide (0.1 mol) and 3,4-dimethylbenzaldehyde (0.1 mol) was stirred in refluxing ethanol (30 mL) for 2 h to afford the title compound (0.085 mol, yield 85%). Single crystals suitable for X-ray measurements were obtained by recrystallization of a solution of the title compound in ethanol at room temperature.

Refinement top

H atoms were fixed geometrically and allowed to ride on their attached atoms, with C—H distances = 0.93-0.97 Å; N-H = 0.86Å, and with Uiso = 1.2Ueq(C,N) or 1.2Ueq(Cmethyl).

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound showing 30% probability displacement ellipsoids and the atom-numbering scheme.
1-(3,4-Dimethylbenzylidene)-4-ethylthiosemicarbazide top
Crystal data top
C12H17N3SF(000) = 504
Mr = 235.35Dx = 1.189 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2429 reflections
a = 8.6659 (17) Åθ = 3.3–27.5°
b = 15.207 (3) ŵ = 0.23 mm1
c = 9.993 (2) ÅT = 293 K
β = 93.47 (3)°Block, colorless
V = 1314.5 (5) Å30.22 × 0.20 × 0.18 mm
Z = 4
Data collection top
Bruker SMART CCD
diffractometer
2429 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.056
graphiteθmax = 27.5°, θmin = 3.3°
φ and ω scansh = 1111
12215 measured reflectionsk = 1919
3006 independent reflectionsl = 1211
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.065Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.206H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.1293P)2 + 0.2681P]
where P = (Fo2 + 2Fc2)/3
3006 reflections(Δ/σ)max < 0.001
145 parametersΔρmax = 0.39 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
C12H17N3SV = 1314.5 (5) Å3
Mr = 235.35Z = 4
Monoclinic, P21/cMo Kα radiation
a = 8.6659 (17) ŵ = 0.23 mm1
b = 15.207 (3) ÅT = 293 K
c = 9.993 (2) Å0.22 × 0.20 × 0.18 mm
β = 93.47 (3)°
Data collection top
Bruker SMART CCD
diffractometer
2429 reflections with I > 2σ(I)
12215 measured reflectionsRint = 0.056
3006 independent reflectionsθmax = 27.5°
Refinement top
R[F2 > 2σ(F2)] = 0.065H-atom parameters constrained
wR(F2) = 0.206Δρmax = 0.39 e Å3
S = 1.05Δρmin = 0.34 e Å3
3006 reflectionsAbsolute structure: ?
145 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

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) top
xyzUiso*/Ueq
S10.84996 (8)0.11266 (4)0.92188 (6)0.0702 (3)
N11.02915 (18)0.11306 (10)1.28935 (16)0.0480 (4)
N20.9879 (2)0.08927 (11)1.15935 (16)0.0532 (4)
H2A1.02350.04151.12690.064*
C91.1228 (2)0.06157 (13)1.35388 (19)0.0513 (4)
H9A1.15740.01151.31140.062*
N30.8377 (2)0.21192 (12)1.14109 (18)0.0581 (4)
H3A0.86300.21931.22490.070*
C41.1328 (3)0.15253 (16)1.5627 (2)0.0597 (5)
H4A1.06910.19471.52060.072*
C81.2782 (2)0.01920 (13)1.5576 (2)0.0544 (5)
H8A1.31200.02931.51080.065*
C31.1773 (2)0.07867 (13)1.49181 (19)0.0487 (4)
C100.8916 (2)0.14075 (13)1.08270 (19)0.0485 (4)
C71.3299 (2)0.03031 (14)1.6911 (2)0.0571 (5)
C61.2793 (3)0.10241 (17)1.7607 (2)0.0644 (6)
C51.1829 (3)0.16286 (18)1.6946 (2)0.0708 (6)
H5A1.15110.21201.74090.085*
C21.4415 (3)0.0353 (2)1.7562 (3)0.0837 (8)
H2B1.46510.01881.84800.126*
H2C1.53480.03601.70920.126*
H2D1.39560.09271.75300.126*
C120.5844 (3)0.2822 (2)1.1272 (4)0.0950 (9)
H12A0.52390.32651.08000.143*
H12B0.59350.29631.22100.143*
H12C0.53480.22611.11490.143*
C110.7391 (3)0.27866 (18)1.0749 (3)0.0787 (7)
H11A0.72890.26630.97960.094*
H11B0.78810.33571.08680.094*
C11.3292 (4)0.1167 (3)1.9069 (3)0.0973 (11)
H1B1.28320.16981.93800.146*
H1C1.43970.12161.91660.146*
H1D1.29620.06791.95890.146*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0834 (5)0.0734 (4)0.0509 (4)0.0196 (3)0.0188 (3)0.0005 (2)
N10.0472 (8)0.0524 (8)0.0437 (8)0.0018 (6)0.0027 (6)0.0016 (6)
N20.0575 (9)0.0541 (8)0.0464 (8)0.0123 (7)0.0088 (7)0.0005 (7)
C90.0536 (10)0.0496 (9)0.0496 (10)0.0050 (7)0.0049 (8)0.0006 (8)
N30.0575 (9)0.0611 (10)0.0554 (9)0.0163 (8)0.0018 (7)0.0074 (7)
C40.0582 (11)0.0668 (13)0.0535 (11)0.0141 (9)0.0015 (8)0.0024 (9)
C80.0552 (10)0.0493 (9)0.0572 (11)0.0028 (8)0.0075 (8)0.0059 (8)
C30.0461 (9)0.0515 (9)0.0481 (9)0.0020 (7)0.0019 (7)0.0045 (8)
C100.0414 (9)0.0526 (9)0.0510 (10)0.0036 (7)0.0019 (7)0.0086 (8)
C70.0505 (10)0.0641 (11)0.0554 (11)0.0114 (8)0.0088 (8)0.0156 (9)
C60.0523 (11)0.0943 (16)0.0459 (11)0.0092 (10)0.0025 (8)0.0010 (10)
C50.0677 (14)0.0861 (16)0.0580 (12)0.0112 (11)0.0003 (10)0.0162 (11)
C20.0802 (16)0.0911 (18)0.0768 (16)0.0046 (13)0.0208 (13)0.0262 (14)
C120.0636 (15)0.0908 (19)0.128 (3)0.0270 (14)0.0117 (15)0.0062 (18)
C110.0817 (16)0.0739 (15)0.0810 (16)0.0347 (13)0.0081 (12)0.0185 (12)
C10.089 (2)0.150 (3)0.0508 (14)0.0023 (18)0.0132 (13)0.0072 (15)
Geometric parameters (Å, °) top
S1—C101.681 (2)C7—C21.509 (3)
N1—C91.275 (2)C6—C51.383 (3)
N1—N21.375 (2)C6—C11.514 (3)
N2—C101.349 (2)C5—H5A0.9300
N2—H2A0.8600C2—H2B0.9600
C9—C31.453 (3)C2—H2C0.9600
C9—H9A0.9300C2—H2D0.9600
N3—C101.328 (3)C12—C111.468 (4)
N3—C111.459 (3)C12—H12A0.9600
N3—H3A0.8600C12—H12B0.9600
C4—C51.371 (3)C12—H12C0.9600
C4—C31.395 (3)C11—H11A0.9700
C4—H4A0.9300C11—H11B0.9700
C8—C71.392 (3)C1—H1B0.9600
C8—C31.395 (3)C1—H1C0.9600
C8—H8A0.9300C1—H1D0.9600
C7—C61.384 (3)
C9—N1—N2115.95 (16)C4—C5—C6122.0 (2)
C10—N2—N1120.03 (16)C4—C5—H5A119.0
C10—N2—H2A120.0C6—C5—H5A119.0
N1—N2—H2A120.0C7—C2—H2B109.5
N1—C9—C3122.03 (18)C7—C2—H2C109.5
N1—C9—H9A119.0H2B—C2—H2C109.5
C3—C9—H9A119.0C7—C2—H2D109.5
C10—N3—C11125.4 (2)H2B—C2—H2D109.5
C10—N3—H3A117.3H2C—C2—H2D109.5
C11—N3—H3A117.3C11—C12—H12A109.5
C5—C4—C3119.9 (2)C11—C12—H12B109.5
C5—C4—H4A120.0H12A—C12—H12B109.5
C3—C4—H4A120.0C11—C12—H12C109.5
C7—C8—C3121.9 (2)H12A—C12—H12C109.5
C7—C8—H8A119.0H12B—C12—H12C109.5
C3—C8—H8A119.0N3—C11—C12112.7 (2)
C8—C3—C4117.90 (18)N3—C11—H11A109.0
C8—C3—C9119.30 (18)C12—C11—H11A109.0
C4—C3—C9122.80 (18)N3—C11—H11B109.0
N3—C10—N2116.46 (17)C12—C11—H11B109.0
N3—C10—S1124.51 (14)H11A—C11—H11B107.8
N2—C10—S1119.02 (15)C6—C1—H1B109.5
C6—C7—C8119.00 (19)C6—C1—H1C109.5
C6—C7—C2121.4 (2)H1B—C1—H1C109.5
C8—C7—C2119.6 (2)C6—C1—H1D109.5
C5—C6—C7119.1 (2)H1B—C1—H1D109.5
C5—C6—C1119.6 (2)H1C—C1—H1D109.5
C7—C6—C1121.2 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···S1i0.862.653.4929 (18)168
Symmetry codes: (i) −x+2, −y, −z+2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N2—H2A···S1i0.862.653.4929 (18)168
Symmetry codes: (i) −x+2, −y, −z+2.
references
References top

Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Casas, J. S., Garcia-Tasende, M. S. & Sordo, J. (2000). Coord. Chem. Rev. 209, 197–261.

Habermehl, N. C., Angus, P. M. & Kilah, N. L. (2006). Inorg. Chem. 45, 1445–1462.

Li, Y.-F. & Jian, F.-F. (2010). Acta Cryst. E66, o1399.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.