Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jan 22;67(Pt 2):o449. doi: 10.1107/S160053681100198X

1-Benzyl­idene­amino-3-(4-methyl­phen­yl)thio­urea

Yan-Ling Zhang a, Zhi-Hong Xu a, Fu-Juan Zhang a, Feng-Ling Yang a,*
PMCID: PMC3051669  PMID: 21523112

Abstract

In the title compound, C15H15N3S, the almost planar 2-benzyl­idenehydrazinecarbothio­amide unit (r.m.s. deviation = 0.0351 Å) is aligned at a dihedral angle of 64.42 (6)° with respect to the plane of the tolyl ring. The mol­ecule exhibits an E configuration for the azomethine linkage. In the crystal, inter­molecular N—H⋯S hydrogen bonds about centers of inversion lead to the formation of dimers.

Related literature

For biological applications of thio­semicarbazones, see: Hu et al. (2006).graphic file with name e-67-0o449-scheme1.jpg

Experimental

Crystal data

  • C15H15N3S

  • M r = 269.36

  • Monoclinic, Inline graphic

  • a = 10.2359 (3) Å

  • b = 16.0648 (3) Å

  • c = 9.9703 (3) Å

  • β = 117.154 (4)°

  • V = 1458.81 (7) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 1.88 mm−1

  • T = 293 K

  • 0.30 × 0.20 × 0.18 mm

Data collection

  • Oxford Diffraction Xcalibur Eos Gemini diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.603, T max = 0.729

  • 12637 measured reflections

  • 2605 independent reflections

  • 2253 reflections with I > 2σ(I)

  • R int = 0.026

  • Standard reflections: 0

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.120

  • S = 1.05

  • 2605 reflections

  • 181 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.19 e Å−3

  • Δρmin = −0.21 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 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: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053681100198X/ng5104sup1.cif

e-67-0o449-sup1.cif (17.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681100198X/ng5104Isup2.hkl

e-67-0o449-Isup2.hkl (128KB, 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
N2—H2⋯S1i 0.88 (2) 2.48 (2) 3.3522 (15) 170.3 (17)

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the Natural Science Foundation of the Education Department of Henan Province (2010B150029), the Natural Science Foundation of Henan Province (082300420110) and the Scientific Research Foundation of Xuchang University of Henan Province (2009086) for supporting this work.

supplementary crystallographic information

Comment

Thiosemicarbazones have attracted our attention because of their biological applications (Hu et al., 2006). A few single-crystal reports about them are presented. Detailed information on their molecular and crystal structures is necessary to understand their anticancer activity. The molecular structure of (I) is shown in Fig 1. The molecules exhibit an E configuration.The thiosemicarbazide and benzaldehyde unit are located on opposite sides of the N1=C7 bond.The 2-benzylidenehydrazinecarbothioamide unit has a planar configuration and subtends an angle of 64.42 (6)° with respect to the plane of the tolyl ring.In the crystal structure of the title compound, there is N(2)—H(2)···S(1)#1 hydrogen-bond interactions in molecules which leads to a supramolecular architecture (Fig. 2).

Experimental

N-(p-Tolyl)hydrazinecarbothioamide (2.7 g,15 mmol) and benzaldehyde (1.6 g, 15 mmol) was dissolved in 95% ethanol (20 ml) and the solution was refluxed for 6.5 h. Fine colorless crystals appeared on cooling. They were filtered and washed by 95% ethanol to give 2.6 g of the title compound in 65% yield. Single crystals suitable for X-ray measurements were obtained from 2-propanol by slow evaporation at room temperature.

Refinement

H atoms were placed in calculated positions with C—H = 0.93–0.96 and N—H = 0.88–0.90 Å, and refined using a riding model, Uiso(H) = 1.5Ueq(C) for methyl H atoms and 1.2Ueq(C,N).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with displacement ellipsoids drawn at 30% probability level.

Fig. 2.

Fig. 2.

The packing diagram of the title compound. Intermolecular hydrogen bonds are shown as dashed line.

Crystal data

C15H15N3S F(000) = 568
Mr = 269.36 Dx = 1.226 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54184 Å
Hall symbol: -P 2ybc Cell parameters from 7009 reflections
a = 10.2359 (3) Å θ = 4.9–72.1°
b = 16.0648 (3) Å µ = 1.88 mm1
c = 9.9703 (3) Å T = 293 K
β = 117.154 (4)° Prismatic, colorless
V = 1458.81 (7) Å3 0.30 × 0.20 × 0.18 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur Eos Gemini diffractometer 2605 independent reflections
Radiation source: fine-focus sealed tube 2253 reflections with I > 2σ(I)
graphite Rint = 0.026
ω scans θmax = 67.1°, θmin = 4.9°
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) h = −12→12
Tmin = 0.603, Tmax = 0.729 k = −19→19
12637 measured reflections l = −8→11

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.120 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0727P)2 + 0.1569P] where P = (Fo2 + 2Fc2)/3
2605 reflections (Δ/σ)max < 0.001
181 parameters Δρmax = 0.19 e Å3
0 restraints Δρmin = −0.21 e Å3

Special details

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
S1 0.13263 (6) 0.10810 (3) 0.02008 (5) 0.0727 (2)
N1 0.15900 (15) −0.00305 (8) 0.37897 (15) 0.0546 (3)
N2 0.12114 (16) 0.01805 (8) 0.23296 (16) 0.0566 (3)
N3 0.28187 (16) 0.12678 (9) 0.31818 (17) 0.0599 (4)
C1 0.2093 (2) −0.05346 (12) 0.6752 (2) 0.0684 (5)
H1 0.2567 −0.0052 0.6694 0.082*
C2 0.2298 (3) −0.08202 (15) 0.8131 (2) 0.0815 (6)
H2A 0.2905 −0.0528 0.9000 0.098*
C3 0.1610 (3) −0.15388 (14) 0.8239 (2) 0.0798 (6)
H3A 0.1763 −0.1736 0.9177 0.096*
C4 0.0699 (3) −0.19596 (13) 0.6949 (2) 0.0765 (5)
H4 0.0226 −0.2441 0.7014 0.092*
C5 0.0481 (2) −0.16751 (11) 0.5560 (2) 0.0667 (4)
H5 −0.0140 −0.1964 0.4693 0.080*
C6 0.11855 (18) −0.09582 (10) 0.5445 (2) 0.0560 (4)
C7 0.09253 (18) −0.06621 (10) 0.39603 (19) 0.0569 (4)
H7 0.0252 −0.0943 0.3110 0.068*
C8 0.18293 (17) 0.08400 (9) 0.20078 (19) 0.0532 (4)
C9 0.35959 (17) 0.19777 (10) 0.30466 (18) 0.0542 (4)
C10 0.4599 (2) 0.18975 (13) 0.2504 (3) 0.0838 (6)
H10 0.4801 0.1375 0.2241 0.101*
C11 0.5311 (3) 0.25904 (16) 0.2346 (3) 0.0938 (8)
H11 0.5983 0.2529 0.1965 0.113*
C12 0.5053 (2) 0.33670 (13) 0.2737 (2) 0.0750 (5)
C13 0.4092 (2) 0.34307 (11) 0.3338 (3) 0.0790 (5)
H13 0.3933 0.3948 0.3656 0.095*
C14 0.3353 (2) 0.27444 (11) 0.3483 (2) 0.0670 (5)
H14 0.2692 0.2804 0.3877 0.080*
C15 0.5825 (3) 0.41238 (18) 0.2529 (3) 0.1188 (11)
H15B 0.6778 0.3966 0.2653 0.178*
H15C 0.5928 0.4538 0.3265 0.178*
H15A 0.5257 0.4347 0.1536 0.178*
H2 0.054 (2) −0.0105 (12) 0.158 (2) 0.067 (5)*
H3 0.294 (2) 0.1122 (12) 0.410 (3) 0.069 (6)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0880 (4) 0.0664 (3) 0.0596 (3) −0.0262 (2) 0.0302 (2) 0.00300 (19)
N1 0.0597 (7) 0.0492 (7) 0.0585 (8) 0.0007 (5) 0.0303 (6) 0.0018 (5)
N2 0.0642 (8) 0.0480 (7) 0.0573 (8) −0.0075 (6) 0.0275 (7) 0.0007 (6)
N3 0.0670 (8) 0.0561 (7) 0.0596 (8) −0.0104 (6) 0.0315 (7) −0.0027 (6)
C1 0.0754 (11) 0.0668 (10) 0.0659 (11) −0.0117 (8) 0.0349 (9) −0.0038 (8)
C2 0.0902 (14) 0.0930 (14) 0.0586 (11) −0.0119 (11) 0.0317 (10) −0.0073 (10)
C3 0.0928 (14) 0.0919 (14) 0.0675 (12) 0.0027 (11) 0.0476 (11) 0.0111 (10)
C4 0.0926 (14) 0.0691 (11) 0.0825 (13) −0.0089 (10) 0.0527 (12) 0.0085 (9)
C5 0.0784 (11) 0.0588 (9) 0.0701 (11) −0.0105 (8) 0.0401 (9) −0.0037 (8)
C6 0.0627 (9) 0.0510 (8) 0.0620 (9) 0.0003 (6) 0.0352 (8) −0.0008 (7)
C7 0.0656 (9) 0.0496 (8) 0.0593 (9) −0.0042 (7) 0.0317 (7) −0.0034 (7)
C8 0.0561 (8) 0.0444 (7) 0.0634 (9) 0.0003 (6) 0.0309 (7) 0.0010 (6)
C9 0.0535 (8) 0.0537 (8) 0.0560 (8) −0.0063 (6) 0.0257 (7) −0.0044 (6)
C10 0.0799 (13) 0.0721 (12) 0.1209 (18) −0.0164 (10) 0.0643 (13) −0.0325 (12)
C11 0.0858 (14) 0.1098 (17) 0.1139 (18) −0.0380 (13) 0.0699 (14) −0.0354 (14)
C12 0.0735 (11) 0.0781 (12) 0.0649 (11) −0.0267 (9) 0.0242 (9) −0.0005 (9)
C13 0.0830 (13) 0.0539 (10) 0.0972 (15) −0.0054 (9) 0.0387 (11) −0.0048 (9)
C14 0.0668 (10) 0.0599 (10) 0.0840 (12) −0.0036 (8) 0.0427 (9) −0.0096 (8)
C15 0.123 (2) 0.117 (2) 0.1007 (19) −0.0629 (18) 0.0376 (16) 0.0096 (15)

Geometric parameters (Å, °)

S1—C8 1.6776 (17) C5—H5 0.9300
N1—C7 1.276 (2) C6—C7 1.459 (2)
N1—N2 1.367 (2) C7—H7 0.9300
N2—C8 1.346 (2) C9—C14 1.366 (2)
N2—H2 0.88 (2) C9—C10 1.368 (3)
N3—C8 1.336 (2) C10—C11 1.378 (3)
N3—C9 1.432 (2) C10—H10 0.9300
N3—H3 0.90 (2) C11—C12 1.368 (3)
C1—C2 1.371 (3) C11—H11 0.9300
C1—C6 1.386 (3) C12—C13 1.370 (3)
C1—H1 0.9300 C12—C15 1.515 (3)
C2—C3 1.382 (3) C13—C14 1.381 (3)
C2—H2A 0.9300 C13—H13 0.9300
C3—C4 1.374 (3) C14—H14 0.9300
C3—H3A 0.9300 C15—H15B 0.9600
C4—C5 1.376 (3) C15—H15C 0.9600
C4—H4 0.9300 C15—H15A 0.9600
C5—C6 1.391 (2)
C7—N1—N2 115.46 (14) N3—C8—N2 116.54 (15)
C8—N2—N1 120.89 (14) N3—C8—S1 124.09 (12)
C8—N2—H2 118.7 (13) N2—C8—S1 119.37 (13)
N1—N2—H2 120.4 (13) C14—C9—C10 119.28 (16)
C8—N3—C9 123.97 (14) C14—C9—N3 119.92 (15)
C8—N3—H3 117.3 (13) C10—C9—N3 120.80 (15)
C9—N3—H3 118.6 (13) C9—C10—C11 120.03 (18)
C2—C1—C6 120.59 (18) C9—C10—H10 120.0
C2—C1—H1 119.7 C11—C10—H10 120.0
C6—C1—H1 119.7 C12—C11—C10 121.56 (19)
C1—C2—C3 120.49 (19) C12—C11—H11 119.2
C1—C2—H2A 119.8 C10—C11—H11 119.2
C3—C2—H2A 119.8 C11—C12—C13 117.60 (18)
C4—C3—C2 119.36 (18) C11—C12—C15 120.8 (2)
C4—C3—H3A 120.3 C13—C12—C15 121.6 (2)
C2—C3—H3A 120.3 C12—C13—C14 121.51 (19)
C3—C4—C5 120.53 (18) C12—C13—H13 119.2
C3—C4—H4 119.7 C14—C13—H13 119.2
C5—C4—H4 119.7 C9—C14—C13 119.93 (17)
C4—C5—C6 120.38 (18) C9—C14—H14 120.0
C4—C5—H5 119.8 C13—C14—H14 120.0
C6—C5—H5 119.8 C12—C15—H15B 109.5
C1—C6—C5 118.64 (16) C12—C15—H15C 109.5
C1—C6—C7 121.86 (15) H15B—C15—H15C 109.5
C5—C6—C7 119.48 (15) C12—C15—H15A 109.5
N1—C7—C6 122.22 (15) H15B—C15—H15A 109.5
N1—C7—H7 118.9 H15C—C15—H15A 109.5
C6—C7—H7 118.9
C7—N1—N2—C8 179.41 (15) N1—N2—C8—N3 0.1 (2)
C6—C1—C2—C3 0.4 (3) N1—N2—C8—S1 −179.63 (11)
C1—C2—C3—C4 −0.9 (4) C8—N3—C9—C14 113.67 (19)
C2—C3—C4—C5 0.6 (3) C8—N3—C9—C10 −67.3 (2)
C3—C4—C5—C6 0.2 (3) C14—C9—C10—C11 −2.5 (3)
C2—C1—C6—C5 0.4 (3) N3—C9—C10—C11 178.4 (2)
C2—C1—C6—C7 178.92 (18) C9—C10—C11—C12 0.7 (4)
C4—C5—C6—C1 −0.7 (3) C10—C11—C12—C13 2.0 (4)
C4—C5—C6—C7 −179.28 (17) C10—C11—C12—C15 −178.9 (2)
N2—N1—C7—C6 −178.88 (14) C11—C12—C13—C14 −3.0 (3)
C1—C6—C7—N1 4.7 (3) C15—C12—C13—C14 177.9 (2)
C5—C6—C7—N1 −176.80 (16) C10—C9—C14—C13 1.6 (3)
C9—N3—C8—N2 179.12 (14) N3—C9—C14—C13 −179.34 (18)
C9—N3—C8—S1 −1.2 (2) C12—C13—C14—C9 1.2 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H2···S1i 0.88 (2) 2.48 (2) 3.3522 (15) 170.3 (17)

Symmetry codes: (i) −x, −y, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5104).

References

  1. Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.
  2. Hu, W.-X., Zhou, W., Xia, C.-N. & Wen, X. (2006). Bioorg. Med. Chem. Lett. 16, 2213–2218. [DOI] [PubMed]
  3. Oxford Diffraction (2010). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S160053681100198X/ng5104sup1.cif

e-67-0o449-sup1.cif (17.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681100198X/ng5104Isup2.hkl

e-67-0o449-Isup2.hkl (128KB, 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

RESOURCES