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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Feb 12;67(Pt 3):o602. doi: 10.1107/S1600536811004557

1-Benzoyl-3,3-bis­(2-methyl­prop­yl)thio­urea

N Selvakumaran a, R Karvembu a,‡, Seik Weng Ng b, Edward R T Tiekink b,*
PMCID: PMC3052116  PMID: 21522360

Abstract

The title compound, C16H24N2OS, is twisted about the central N(H)—C bond with the C—N—C—S torsion angle being 119.6 (3)°. The carbonyl O and thione S atoms are directed to opposite sides of the mol­ecule, a conformation that allows for the formation of a linear supra­molecular chain comprising alternating eight-membered {⋯HNCS}2 and 14-membered {⋯HCNCNCO}2 synthons.

Related literature

For the coordinating ability of N,N-dialkyl-N′-benzoyl­thio­ureas; see: Binzet et al. (2009 ▶); Gunasekaran et al. (2010 ▶); Sacht et al. (2000 ▶). For the utility of Cd derivatives to serve as synthetic precursors for CdS nanoparticles, see: Bruce et al. (2007 ▶). For their biological activity, see: Arslan et al. (2006 ▶). For related structures, see: Gunasekaran et al. (2010a ▶,b ▶).graphic file with name e-67-0o602-scheme1.jpg

Experimental

Crystal data

  • C16H24N2OS

  • M r = 292.43

  • Triclinic, Inline graphic

  • a = 8.9331 (10) Å

  • b = 10.1023 (9) Å

  • c = 11.0725 (12) Å

  • α = 105.776 (9)°

  • β = 112.734 (10)°

  • γ = 100.782 (9)°

  • V = 837.47 (19) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.19 mm−1

  • T = 295 K

  • 0.35 × 0.30 × 0.25 mm

Data collection

  • Agilent Supernova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.936, T max = 0.954

  • 6265 measured reflections

  • 3693 independent reflections

  • 2232 reflections with I > 2σ(I)

  • R int = 0.025

Refinement

  • R[F 2 > 2σ(F 2)] = 0.074

  • wR(F 2) = 0.219

  • S = 1.04

  • 3693 reflections

  • 181 parameters

  • 12 restraints

  • H-atom parameters constrained

  • Δρmax = 0.86 e Å−3

  • Δρmin = −0.58 e Å−3

Data collection: CrysAlis PRO (Agilent, 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: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811004557/ez2230sup1.cif

e-67-0o602-sup1.cif (18.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004557/ez2230Isup2.hkl

e-67-0o602-Isup2.hkl (181KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N1—H1⋯S1i 0.88 2.74 3.586 (3) 162
C9—H9a⋯O1ii 0.97 2.49 3.424 (5) 162

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

Acknowledgments

NS thanks the NITT for a Fellowship. The authors thank the University of Malaya for supporting this study.

supplementary crystallographic information

Comment

N,N-Dialkyl-N'-benzoylthioureas are versatile ligands which can coordinate to transition metal centres either as neutral species or in an anionic form. The complexation capacity of thiourea derivatives has been reported in several studies (Binzet et al., 2009; Gunasekaran et al., 2010). Chiral and achiral platinum(II) complexes of these ligands have been used as chemotherapeutic agents (Sacht et al., 2000) while cadmium(II) complexes of N,N-diethyl-N'-benzoylthiourea have been used as single-source precursors for the preparation of CdS nanoparticles (Bruce et al., 2007). In addition, thioureas have been shown to possess anti-tubercular, anti-helmintic, anti-bacterial, insecticidal and rodenticidal properties (Arslan et al., 2006). In continuation of structural studies of these derivatives (Gunasekaran et al., 2010a; Gunasekaran et al., 2010b), the title compound, (I), was investigated.

In (I), Fig. 1, the molecule exhibits a significant twist about the central N(H)–C bond as seen in the value of the C7–N1–C8–S1 torsion angle of 119.6 (3) °. This arrangement causes the carbonyl-O and thione-S atoms to lie on opposite sides of the molecule. Similarly, the carbonyl and N–H groups are directed away from each other. This conformation allows for the formation of N–H···S hydrogen bonds, Table 1, via an eight-membered {···HNCS}2 ring which has the shape of an elongated chair. These are connected into supramolecular chains along [1 1 1] via C–H···O contacts that close 14-membered {···HCNCNCO}2 synthons, also adopting the shape of an elongated chair, Table 1 and Fig. 2. Chains are arranged into layers via weak π···π interactions [Cg(C1–C6)···Cg(C1–C6)i = 3.806 (3) Å for i: 2 - x, 1 - y, 2 - z] and these stack as shown in Fig. 3.

Experimental

A solution of benzoyl chloride (0.7029 g, 5 mmol) in acetone (50 ml) was added drop wise to a suspension of potassium thiocyanate (0.4859 g, 5 mmol) in anhydrous acetone (50 ml). The reaction mixture was heated under reflux for 45 min. and then cooled to room temperature. A solution of diisobutyl amine (0.6462 g, 5 mmol) in acetone (30 ml) was added and the resulting mixture was stirred for 2 h. Hydrochloric acid (0.1 N, 300 ml) was added and the resulting white solid was filtered, washed with water and dried in vacuo. Single crystals for X-ray diffraction were grown at room temperature from an acetonitrile solution of the compound. Yield 72%; M.Pt. 415 K. FT—IR (KBr) ν(N—H) 3268, ν(C═O) 1688, ν(C=S) 1264 cm-1.

Refinement

The H-atoms were placed in calculated positions (N—H = 0.88; C—H 0.93 to 0.98 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2 to 1.5Uequiv(N, C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 35% probability level.

Fig. 2.

Fig. 2.

Supramolecular chain in (I) mediated by N–H···S hydrogen bonds and C–H···O contacts, shown as orange and blue dashed lines, respectively.

Fig. 3.

Fig. 3.

View in projection down the b axis of the unit cell contents of (I). The N–H···S hydrogen bonds and C–H···O contacts are shown as orange and blue dashed lines, respectively.

Crystal data

C16H24N2OS Z = 2
Mr = 292.43 F(000) = 316
Triclinic, P1 Dx = 1.160 Mg m−3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.9331 (10) Å Cell parameters from 1845 reflections
b = 10.1023 (9) Å θ = 2.2–29.2°
c = 11.0725 (12) Å µ = 0.19 mm−1
α = 105.776 (9)° T = 295 K
β = 112.734 (10)° Block, colourless
γ = 100.782 (9)° 0.35 × 0.30 × 0.25 mm
V = 837.47 (19) Å3

Data collection

Agilent Supernova Dual diffractometer with an Atlas detector 3693 independent reflections
Radiation source: SuperNova (Mo) X-ray Source 2232 reflections with I > 2σ(I)
Mirror Rint = 0.025
Detector resolution: 10.4041 pixels mm-1 θmax = 27.5°, θmin = 2.2°
ω scans h = −10→11
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) k = −13→12
Tmin = 0.936, Tmax = 0.954 l = −14→12
6265 measured reflections

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)] = 0.074 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.219 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.078P)2 + 0.7593P] where P = (Fo2 + 2Fc2)/3
3693 reflections (Δ/σ)max = 0.001
181 parameters Δρmax = 0.86 e Å−3
12 restraints Δρmin = −0.58 e Å−3

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 > 2σ(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 0.74828 (14) 0.92803 (11) 0.99096 (12) 0.0711 (4)
O1 0.6998 (3) 0.5295 (2) 0.7153 (3) 0.0585 (7)
N1 0.8690 (3) 0.7638 (3) 0.8494 (3) 0.0512 (7)
H1 0.9753 0.8236 0.8909 0.061*
N2 0.6172 (3) 0.7981 (3) 0.7098 (3) 0.0515 (7)
C1 0.9961 (4) 0.5699 (3) 0.8524 (3) 0.0431 (7)
C2 0.9697 (5) 0.4222 (4) 0.8112 (4) 0.0535 (9)
H2 0.8597 0.3566 0.7487 0.064*
C3 1.1045 (5) 0.3706 (4) 0.8615 (5) 0.0653 (11)
H3 1.0847 0.2708 0.8335 0.078*
C4 1.2664 (5) 0.4656 (5) 0.9522 (5) 0.0669 (11)
H4 1.3568 0.4306 0.9866 0.080*
C5 1.2961 (5) 0.6133 (5) 0.9929 (5) 0.0661 (11)
H5 1.4069 0.6780 1.0542 0.079*
C6 1.1618 (4) 0.6657 (4) 0.9431 (4) 0.0538 (9)
H6 1.1826 0.7656 0.9705 0.065*
C7 0.8421 (4) 0.6165 (3) 0.7986 (3) 0.0426 (7)
C8 0.7372 (4) 0.8250 (3) 0.8392 (4) 0.0513 (9)
C9 0.6351 (4) 0.7432 (3) 0.5811 (4) 0.0526 (9)
H9A 0.5352 0.6588 0.5122 0.063*
H9B 0.7353 0.7118 0.6035 0.063*
C10 0.6535 (5) 0.8564 (4) 0.5150 (4) 0.0654 (11)
H10 0.5463 0.8792 0.4831 0.079*
C11 0.6790 (7) 0.7906 (5) 0.3856 (4) 0.0892 (15)
H11A 0.5849 0.7025 0.3204 0.134*
H11B 0.7847 0.7691 0.4149 0.134*
H11C 0.6835 0.8587 0.3403 0.134*
C12 0.7998 (6) 0.9970 (4) 0.6237 (5) 0.0877 (15)
H12A 0.8091 1.0661 0.5801 0.132*
H12B 0.9057 0.9765 0.6583 0.132*
H12C 0.7765 1.0367 0.7012 0.132*
C13 0.4659 (4) 0.8426 (4) 0.6909 (5) 0.0662 (11)
H13A 0.4206 0.8536 0.6005 0.079*
H13B 0.5025 0.9377 0.7640 0.079*
C14 0.3240 (5) 0.7441 (4) 0.6949 (7) 0.106 (2)
H14 0.3640 0.7625 0.7957 0.127*
C15 0.1645 (5) 0.7914 (5) 0.6518 (6) 0.0888 (15)
H15A 0.1979 0.8950 0.6987 0.133*
H15B 0.0863 0.7435 0.6785 0.133*
H15C 0.1094 0.7655 0.5512 0.133*
C16 0.2816 (6) 0.5830 (4) 0.6261 (6) 0.0816 (13)
H16A 0.3853 0.5586 0.6554 0.122*
H16B 0.2264 0.5542 0.5251 0.122*
H16C 0.2058 0.5330 0.6536 0.122*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0676 (7) 0.0507 (6) 0.0765 (7) 0.0191 (5) 0.0294 (6) 0.0036 (5)
O1 0.0434 (13) 0.0383 (13) 0.0653 (16) 0.0071 (11) 0.0031 (12) 0.0157 (12)
N1 0.0344 (14) 0.0355 (15) 0.0622 (18) 0.0091 (12) 0.0100 (13) 0.0078 (13)
N2 0.0364 (14) 0.0400 (15) 0.0659 (19) 0.0137 (12) 0.0144 (14) 0.0156 (14)
C1 0.0428 (17) 0.0444 (18) 0.0423 (17) 0.0167 (15) 0.0181 (14) 0.0176 (14)
C2 0.054 (2) 0.0427 (19) 0.059 (2) 0.0190 (16) 0.0215 (17) 0.0169 (17)
C3 0.069 (3) 0.054 (2) 0.088 (3) 0.034 (2) 0.040 (2) 0.034 (2)
C4 0.055 (2) 0.077 (3) 0.089 (3) 0.039 (2) 0.035 (2) 0.046 (3)
C5 0.0419 (19) 0.071 (3) 0.077 (3) 0.0192 (19) 0.0186 (18) 0.029 (2)
C6 0.0451 (19) 0.050 (2) 0.060 (2) 0.0171 (16) 0.0180 (16) 0.0193 (17)
C7 0.0417 (17) 0.0384 (17) 0.0383 (16) 0.0125 (14) 0.0111 (14) 0.0128 (14)
C8 0.0403 (17) 0.0325 (17) 0.067 (2) 0.0098 (14) 0.0173 (16) 0.0118 (16)
C9 0.0438 (18) 0.0412 (19) 0.060 (2) 0.0136 (15) 0.0125 (16) 0.0183 (17)
C10 0.055 (2) 0.052 (2) 0.075 (3) 0.0160 (18) 0.0104 (19) 0.032 (2)
C11 0.113 (4) 0.077 (3) 0.071 (3) 0.025 (3) 0.033 (3) 0.038 (3)
C12 0.092 (3) 0.052 (3) 0.089 (3) 0.000 (2) 0.021 (3) 0.030 (2)
C13 0.046 (2) 0.057 (2) 0.089 (3) 0.0247 (18) 0.022 (2) 0.027 (2)
C14 0.065 (3) 0.072 (3) 0.203 (7) 0.033 (3) 0.070 (4) 0.065 (4)
C15 0.060 (3) 0.097 (4) 0.139 (5) 0.039 (3) 0.057 (3) 0.060 (4)
C16 0.071 (3) 0.057 (3) 0.113 (4) 0.012 (2) 0.047 (3) 0.027 (3)

Geometric parameters (Å, °)

S1—C8 1.673 (4) C9—H9B 0.9700
O1—C7 1.214 (4) C10—C12 1.528 (4)
N1—C7 1.377 (4) C10—C11 1.529 (4)
N1—C8 1.410 (4) C10—H10 0.9800
N1—H1 0.8800 C11—H11A 0.9600
N2—C8 1.330 (4) C11—H11B 0.9600
N2—C13 1.461 (4) C11—H11C 0.9600
N2—C9 1.464 (5) C12—H12A 0.9600
C1—C2 1.380 (5) C12—H12B 0.9600
C1—C6 1.386 (5) C12—H12C 0.9600
C1—C7 1.493 (4) C13—C14 1.482 (4)
C2—C3 1.381 (5) C13—H13A 0.9700
C2—H2 0.9300 C13—H13B 0.9700
C3—C4 1.362 (6) C14—C16 1.498 (4)
C3—H3 0.9300 C14—C15 1.530 (4)
C4—C5 1.376 (6) C14—H14 0.9800
C4—H4 0.9300 C15—H15A 0.9600
C5—C6 1.382 (5) C15—H15B 0.9600
C5—H5 0.9300 C15—H15C 0.9600
C6—H6 0.9300 C16—H16A 0.9600
C9—C10 1.533 (4) C16—H16B 0.9600
C9—H9A 0.9700 C16—H16C 0.9600
C7—N1—C8 124.2 (3) C12—C10—H10 108.2
C7—N1—H1 117.9 C11—C10—H10 108.2
C8—N1—H1 117.9 C9—C10—H10 108.2
C8—N2—C13 120.0 (3) C10—C11—H11A 109.5
C8—N2—C9 124.2 (3) C10—C11—H11B 109.5
C13—N2—C9 115.2 (3) H11A—C11—H11B 109.5
C2—C1—C6 118.6 (3) C10—C11—H11C 109.5
C2—C1—C7 117.4 (3) H11A—C11—H11C 109.5
C6—C1—C7 124.0 (3) H11B—C11—H11C 109.5
C1—C2—C3 120.9 (4) C10—C12—H12A 109.5
C1—C2—H2 119.6 C10—C12—H12B 109.5
C3—C2—H2 119.6 H12A—C12—H12B 109.5
C4—C3—C2 120.1 (4) C10—C12—H12C 109.5
C4—C3—H3 119.9 H12A—C12—H12C 109.5
C2—C3—H3 119.9 H12B—C12—H12C 109.5
C3—C4—C5 120.0 (3) N2—C13—C14 116.6 (3)
C3—C4—H4 120.0 N2—C13—H13A 108.1
C5—C4—H4 120.0 C14—C13—H13A 108.1
C4—C5—C6 120.2 (4) N2—C13—H13B 108.1
C4—C5—H5 119.9 C14—C13—H13B 108.1
C6—C5—H5 119.9 H13A—C13—H13B 107.3
C5—C6—C1 120.2 (3) C13—C14—C16 118.4 (4)
C5—C6—H6 119.9 C13—C14—C15 111.0 (3)
C1—C6—H6 119.9 C16—C14—C15 112.5 (4)
O1—C7—N1 121.4 (3) C13—C14—H14 104.5
O1—C7—C1 122.1 (3) C16—C14—H14 104.5
N1—C7—C1 116.6 (3) C15—C14—H14 104.5
N2—C8—N1 117.1 (3) C14—C15—H15A 109.5
N2—C8—S1 125.9 (3) C14—C15—H15B 109.5
N1—C8—S1 117.1 (3) H15A—C15—H15B 109.5
N2—C9—C10 113.3 (3) C14—C15—H15C 109.5
N2—C9—H9A 108.9 H15A—C15—H15C 109.5
C10—C9—H9A 108.9 H15B—C15—H15C 109.5
N2—C9—H9B 108.9 C14—C16—H16A 109.5
C10—C9—H9B 108.9 C14—C16—H16B 109.5
H9A—C9—H9B 107.7 H16A—C16—H16B 109.5
C12—C10—C11 112.2 (3) C14—C16—H16C 109.5
C12—C10—C9 110.9 (3) H16A—C16—H16C 109.5
C11—C10—C9 109.1 (3) H16B—C16—H16C 109.5
C6—C1—C2—C3 1.4 (5) C13—N2—C8—N1 172.5 (3)
C7—C1—C2—C3 −177.1 (3) C9—N2—C8—N1 −16.3 (5)
C1—C2—C3—C4 −0.5 (6) C13—N2—C8—S1 −9.0 (5)
C2—C3—C4—C5 −0.5 (6) C9—N2—C8—S1 162.2 (3)
C3—C4—C5—C6 0.6 (7) C7—N1—C8—N2 −61.8 (5)
C4—C5—C6—C1 0.4 (6) C7—N1—C8—S1 119.6 (3)
C2—C1—C6—C5 −1.4 (5) C8—N2—C9—C10 −109.9 (4)
C7—C1—C6—C5 177.1 (3) C13—N2—C9—C10 61.7 (4)
C8—N1—C7—O1 15.7 (5) N2—C9—C10—C12 53.6 (4)
C8—N1—C7—C1 −163.6 (3) N2—C9—C10—C11 177.6 (3)
C2—C1—C7—O1 −4.2 (5) C8—N2—C13—C14 −82.1 (5)
C6—C1—C7—O1 177.4 (3) C9—N2—C13—C14 105.9 (4)
C2—C1—C7—N1 175.2 (3) N2—C13—C14—C16 −39.2 (7)
C6—C1—C7—N1 −3.3 (5) N2—C13—C14—C15 −171.4 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···S1i 0.88 2.74 3.586 (3) 162
C9—H9a···O1ii 0.97 2.49 3.424 (5) 162

Symmetry codes: (i) −x+2, −y+2, −z+2; (ii) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: EZ2230).

References

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  4. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
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  6. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
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Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811004557/ez2230sup1.cif

e-67-0o602-sup1.cif (18.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004557/ez2230Isup2.hkl

e-67-0o602-Isup2.hkl (181KB, hkl)

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


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