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In the title compound, C15H14N2OS, inter­molecular N—H...S hydrogen bonds link pairs of mol­ecules. The steric hindrance of the o-methyl group restricts the formation of a mol­ecular conjugated plane and π–π stacking. The presence of a hydrogen-bond acceptor atom is more helpful for the thio­urea ligand to promote its stability.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536806032740/jh2028sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536806032740/jh2028Isup2.hkl
Contains datablock I

CCDC reference: 273457

Key indicators

  • Single-crystal X-ray study
  • T = 294 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.039
  • wR factor = 0.109
  • Data-to-parameter ratio = 15.4

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT125_ALERT_4_C No _symmetry_space_group_name_Hall Given ....... ?
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL.

N-Benzoyl-N'-(2-methylphenyl)thiourea top
Crystal data top
C15H14N2OSF(000) = 568
Mr = 270.34Dx = 1.305 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 5.6441 (10) ÅCell parameters from 2356 reflections
b = 25.165 (4) Åθ = 2.7–25.7°
c = 9.6851 (17) ŵ = 0.23 mm1
β = 90.216 (3)°T = 294 K
V = 1375.6 (4) Å3Block, colorless
Z = 40.36 × 0.32 × 0.26 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
2792 independent reflections
Radiation source: fine-focus sealed tube1816 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.029
φ and ω scansθmax = 26.4°, θmin = 1.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 76
Tmin = 0.910, Tmax = 0.942k = 3131
7656 measured reflectionsl = 612
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)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.109H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0498P)2 + 0.1902P]
where P = (Fo2 + 2Fc2)/3
2792 reflections(Δ/σ)max = 0.001
181 parametersΔρmax = 0.18 e Å3
0 restraintsΔρmin = 0.17 e Å3
Special details top

Experimental. The infrared spectrum was recorded in the range of 4000–400?cm-1 on a Nicolet NEXUS 670?F T—IR spectrometer, using KBr pellets. 1H NMR spectrum was obtained on an INOVA-400?MHz superconduction spectrometer, DMSO-d6 was used as the solvent and TMS as internal standard, and the chemical shifts are expressed as delta. Elemental analyses were carried out on a PE-2400 CHN instrument. Melting point determination was performed in an open capillary tube and is uncorrected.

N-Benzoyl-N'-(o-methylphenyl)thiourea Color: colorless, Yield: 87%. Melting Point: 116–118(°C). Elemental analysis (%) found (calcd.): C, 65.45(66.67); H, 4.98(5.19); N, 10.76(10.37). IR (KBr, cm-1): 3268 (N—H), 1670 (C=O), 1586, 1527 (C=C), 1262(C=S), 1154. 1H NMR(delta, p.p.m.): 2.26 (s, 3H, CH3); 7.20–8.00 (m, 9H, C6H5, C6H4); 11.61 (s, 1H, NH); 12.29 (s, 1H, NH).

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
S10.64767 (12)0.44364 (2)0.63254 (6)0.0676 (2)
N10.7095 (3)0.35643 (6)0.47815 (17)0.0486 (4)
H10.657 (4)0.3397 (8)0.406 (2)0.059 (6)*
N20.4401 (3)0.41790 (6)0.39893 (16)0.0483 (4)
H20.388 (4)0.4499 (8)0.409 (2)0.053 (6)*
O10.4452 (3)0.34613 (5)0.25749 (15)0.0696 (5)
C10.6042 (3)0.40303 (7)0.49881 (18)0.0456 (5)
C20.8678 (3)0.32847 (7)0.56687 (18)0.0460 (5)
C30.8358 (3)0.27361 (8)0.57925 (19)0.0486 (5)
C40.9884 (4)0.24641 (9)0.6661 (2)0.0675 (6)
H40.96900.21000.67750.081*
C51.1671 (5)0.27173 (12)0.7357 (2)0.0791 (8)
H51.26520.25260.79490.095*
C61.2022 (4)0.32515 (12)0.7187 (2)0.0747 (7)
H61.32640.34210.76430.090*
C71.0531 (4)0.35382 (9)0.6338 (2)0.0592 (6)
H71.07690.39010.62150.071*
C80.6458 (4)0.24438 (8)0.5012 (2)0.0626 (6)
H8A0.63380.20870.53580.094*
H8B0.68510.24350.40490.094*
H8C0.49700.26230.51310.094*
C90.3601 (4)0.38939 (7)0.28725 (19)0.0488 (5)
C100.1637 (3)0.41274 (7)0.20478 (19)0.0468 (5)
C110.0082 (4)0.45052 (7)0.2554 (2)0.0543 (5)
H110.02680.46350.34470.065*
C120.1745 (4)0.46888 (9)0.1731 (2)0.0645 (6)
H120.27720.49470.20680.077*
C130.2056 (4)0.44941 (9)0.0421 (3)0.0697 (6)
H130.33020.46170.01230.084*
C140.0532 (4)0.41187 (9)0.0087 (2)0.0712 (7)
H140.07420.39870.09760.085*
C150.1302 (4)0.39367 (8)0.0717 (2)0.0611 (6)
H150.23330.36830.03660.073*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.1033 (5)0.0452 (3)0.0542 (3)0.0130 (3)0.0247 (3)0.0140 (2)
N10.0641 (11)0.0384 (9)0.0433 (9)0.0030 (8)0.0099 (8)0.0053 (7)
N20.0682 (11)0.0317 (8)0.0448 (9)0.0049 (8)0.0104 (8)0.0044 (7)
O10.0987 (12)0.0457 (8)0.0642 (9)0.0174 (8)0.0295 (8)0.0185 (7)
C10.0606 (12)0.0349 (9)0.0412 (10)0.0017 (9)0.0029 (9)0.0008 (8)
C20.0492 (11)0.0489 (11)0.0398 (10)0.0061 (9)0.0004 (8)0.0020 (8)
C30.0539 (12)0.0473 (11)0.0446 (11)0.0085 (9)0.0035 (9)0.0018 (9)
C40.0758 (17)0.0599 (13)0.0669 (14)0.0192 (12)0.0004 (12)0.0096 (11)
C50.0760 (18)0.095 (2)0.0660 (16)0.0372 (15)0.0138 (13)0.0017 (14)
C60.0570 (15)0.100 (2)0.0667 (16)0.0151 (13)0.0145 (12)0.0204 (14)
C70.0568 (14)0.0619 (13)0.0589 (13)0.0016 (11)0.0043 (11)0.0087 (10)
C80.0707 (15)0.0443 (11)0.0727 (14)0.0018 (10)0.0010 (11)0.0049 (10)
C90.0670 (13)0.0359 (10)0.0434 (11)0.0001 (9)0.0053 (9)0.0037 (8)
C100.0577 (12)0.0373 (10)0.0453 (11)0.0030 (9)0.0052 (9)0.0008 (8)
C110.0571 (13)0.0509 (12)0.0550 (12)0.0056 (10)0.0018 (10)0.0029 (10)
C120.0534 (14)0.0604 (13)0.0797 (16)0.0064 (10)0.0055 (12)0.0024 (12)
C130.0641 (15)0.0739 (16)0.0710 (16)0.0057 (12)0.0147 (12)0.0123 (13)
C140.0866 (18)0.0725 (15)0.0543 (13)0.0087 (13)0.0186 (12)0.0035 (11)
C150.0776 (15)0.0569 (12)0.0487 (12)0.0114 (11)0.0119 (11)0.0063 (10)
Geometric parameters (Å, º) top
S1—C11.6671 (18)C6—H60.9300
N1—C11.330 (2)C7—H70.9300
N1—C21.424 (2)C8—H8A0.9600
N1—H10.87 (2)C8—H8B0.9600
N2—C91.373 (2)C8—H8C0.9600
N2—C11.388 (2)C9—C101.485 (3)
N2—H20.86 (2)C10—C111.385 (3)
O1—C91.225 (2)C10—C151.388 (3)
C2—C71.384 (3)C11—C121.380 (3)
C2—C31.397 (3)C11—H110.9300
C3—C41.383 (3)C12—C131.371 (3)
C3—C81.502 (3)C12—H120.9300
C4—C51.369 (3)C13—C141.370 (3)
C4—H40.9300C13—H130.9300
C5—C61.369 (4)C14—C151.372 (3)
C5—H50.9300C14—H140.9300
C6—C71.378 (3)C15—H150.9300
C1—N1—C2128.67 (17)C3—C8—H8A109.5
C1—N1—H1113.3 (14)C3—C8—H8B109.5
C2—N1—H1117.4 (13)H8A—C8—H8B109.5
C9—N2—C1128.66 (17)C3—C8—H8C109.5
C9—N2—H2117.9 (13)H8A—C8—H8C109.5
C1—N2—H2113.4 (13)H8B—C8—H8C109.5
N1—C1—N2115.47 (16)O1—C9—N2121.47 (18)
N1—C1—S1126.36 (15)O1—C9—C10121.17 (17)
N2—C1—S1118.16 (14)N2—C9—C10117.36 (16)
C7—C2—C3120.86 (18)C11—C10—C15118.79 (19)
C7—C2—N1121.75 (18)C11—C10—C9123.66 (17)
C3—C2—N1117.33 (17)C15—C10—C9117.49 (18)
C4—C3—C2117.43 (19)C12—C11—C10119.9 (2)
C4—C3—C8120.35 (19)C12—C11—H11120.0
C2—C3—C8122.21 (17)C10—C11—H11120.0
C5—C4—C3121.7 (2)C13—C12—C11120.5 (2)
C5—C4—H4119.2C13—C12—H12119.8
C3—C4—H4119.2C11—C12—H12119.8
C4—C5—C6120.3 (2)C14—C13—C12120.0 (2)
C4—C5—H5119.9C14—C13—H13120.0
C6—C5—H5119.9C12—C13—H13120.0
C5—C6—C7119.8 (2)C13—C14—C15120.0 (2)
C5—C6—H6120.1C13—C14—H14120.0
C7—C6—H6120.1C15—C14—H14120.0
C6—C7—C2119.8 (2)C14—C15—C10120.8 (2)
C6—C7—H7120.1C14—C15—H15119.6
C2—C7—H7120.1C10—C15—H15119.6
C2—N1—C1—N2173.91 (18)N1—C2—C7—C6179.96 (19)
C2—N1—C1—S14.9 (3)C1—N2—C9—O15.6 (3)
C9—N2—C1—N15.0 (3)C1—N2—C9—C10173.57 (18)
C9—N2—C1—S1173.91 (16)O1—C9—C10—C11157.1 (2)
C1—N1—C2—C745.1 (3)N2—C9—C10—C1122.0 (3)
C1—N1—C2—C3137.7 (2)O1—C9—C10—C1520.1 (3)
C7—C2—C3—C43.2 (3)N2—C9—C10—C15160.73 (18)
N1—C2—C3—C4179.58 (18)C15—C10—C11—C120.7 (3)
C7—C2—C3—C8176.17 (19)C9—C10—C11—C12177.87 (19)
N1—C2—C3—C81.0 (3)C10—C11—C12—C131.0 (3)
C2—C3—C4—C51.2 (3)C11—C12—C13—C140.7 (4)
C8—C3—C4—C5178.2 (2)C12—C13—C14—C150.1 (4)
C3—C4—C5—C61.3 (4)C13—C14—C15—C100.2 (4)
C4—C5—C6—C71.7 (4)C11—C10—C15—C140.1 (3)
C5—C6—C7—C20.4 (3)C9—C10—C15—C14177.5 (2)
C3—C2—C7—C62.9 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2···S1i0.86 (2)2.72 (2)3.5326 (18)157.9 (17)
N1—H1···O10.87 (2)1.87 (2)2.614 (2)142.4 (19)
Symmetry code: (i) x+1, y+1, z+1.
 

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