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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jan 14;68(Pt 2):o388. doi: 10.1107/S1600536812000888

Diphenyl­methyl isothio­cyanate

Pei-Hua Zhao a,*, Jun-Jie Liu a, Mei Zhang a, Gui-Zhe Zhao a, Ya-Qing Liu a
PMCID: PMC3275065  PMID: 22347010

Abstract

The asymmetric unit of the title compound, C14H11NS, contains two mol­ecules in which the dihedral angles between the phenyl rings are 77.23 (7) and 86.30 (7)°. No aromatic π–π stacking inter­actions are observed.

Related literature

For the synthetic applications of isothio­cyanates, see: Fernandez et al. (1995); Mukerjee & Ashare (1991); Stephensen & Zaragosa (1997).graphic file with name e-68-0o388-scheme1.jpg

Experimental

Crystal data

  • C14H11NS

  • M r = 225.30

  • Triclinic, Inline graphic

  • a = 9.635 (5) Å

  • b = 10.222 (6) Å

  • c = 11.974 (7) Å

  • α = 98.491 (13)°

  • β = 95.296 (15)°

  • γ = 93.573 (6)°

  • V = 1157.9 (11) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.25 mm−1

  • T = 113 K

  • 0.24 × 0.20 × 0.18 mm

Data collection

  • Rigaku Saturn724 CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) T min = 0.943, T max = 0.957

  • 12035 measured reflections

  • 5430 independent reflections

  • 3169 reflections with I > 2σ(I)

  • R int = 0.042

Refinement

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.079

  • S = 0.89

  • 5430 reflections

  • 289 parameters

  • 2 restraints

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.26 e Å−3

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; 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: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812000888/hb6596sup1.cif

e-68-0o388-sup1.cif (22.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812000888/hb6596Isup2.hkl

e-68-0o388-Isup2.hkl (265.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812000888/hb6596Isup3.cml

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

Acknowledgments

This work was supported financially by the Start-up Foundation and the Youth Foundation of North University of China.

supplementary crystallographic information

Experimental

Diphenylamine (44.0 mmol) was dissolved in absolute ethanol (50.0 ml). Carbon disulfide (440.0 mmol) and triethylamine (44.0 mmol) were added while stirring. The reaction mixture was stirred for 0.5 h at room temperature and then cooled on an ice bath. Di-tert butyl dicarbonate (43.6 mmol) dissolved in absolute ethanol (10.0 ml), was added followed by the immediate addition of a catalytic amount of 1,4-diazabicyclo-[2.2.2]octane (0.88 mmol) in absolute ethanol (10.0 ml). The reaction mixture was kept in the ice bath for 5 min, and was then allowed to room temperature. After the reaction was completed, the solvents were evporated thoroughly in vacuo. The residue obtained was taken up in ether and filtered off, and the filtrate was evaporated in vacuo to afford the crude. The crude was separated through column chromatography on silica gel eluting with petroleum ether- dichloromethane (30:1 v/v) to give the white product. Colourless prisms of the title compound were obtained by slow evaporation of the dichloromethane/n-hexane solutions at room temperature. 1H-NMR(400 MHz, CDCl3, TMS): 6.02 (s, 1H, CH), 7.33–7.42 (m, 10H, Ph—H) p.p.m.. 13C-NMR(100 MHz,CDCl3, TMS): 64.6 (CH), 126.7, 128.4, 129.0, 139.3 (Ph—CH and Ph—C) p.p.m..

Refinement

All the H atoms were positioned geometrically (C—H = 0.95 Å) and refined as riding with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I). Displacement ellipsoids are drawn at the 30% probability level and H atoms are shown as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

The crystal packing for (I).

Crystal data

C14H11NS Z = 4
Mr = 225.30 F(000) = 472
Triclinic, P1 Dx = 1.292 Mg m3
a = 9.635 (5) Å Mo Kα radiation, λ = 0.71073 Å
b = 10.222 (6) Å Cell parameters from 3900 reflections
c = 11.974 (7) Å θ = 1.7–28.0°
α = 98.491 (13)° µ = 0.25 mm1
β = 95.296 (15)° T = 113 K
γ = 93.573 (6)° Prism, colorless
V = 1157.9 (11) Å3 0.24 × 0.20 × 0.18 mm

Data collection

Rigaku Saturn724 CCD diffractometer 5430 independent reflections
Radiation source: rotating anode 3169 reflections with I > 2σ(I)
multilayer Rint = 0.042
Detector resolution: 14.22 pixels mm-1 θmax = 27.9°, θmin = 1.7°
ω and φ scans h = −12→12
Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) k = −13→13
Tmin = 0.943, Tmax = 0.957 l = −15→12
12035 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)] = 0.034 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.079 H-atom parameters constrained
S = 0.89 w = 1/[σ2(Fo2) + (0.0253P)2] where P = (Fo2 + 2Fc2)/3
5430 reflections (Δ/σ)max = 0.003
289 parameters Δρmax = 0.20 e Å3
2 restraints Δρmin = −0.26 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 0.10665 (4) 0.73024 (4) 0.96006 (4) 0.03299 (12)
S2 0.11876 (4) 1.01973 (4) 0.18909 (4) 0.03186 (12)
N1 0.10403 (14) 0.46640 (15) 0.86731 (12) 0.0375 (4)
N2 0.27245 (15) 0.85453 (13) 0.30434 (11) 0.0353 (4)
C1 0.14265 (15) 0.41926 (16) 0.63396 (13) 0.0266 (4)
H1 0.1367 0.5072 0.6711 0.032*
C2 0.15692 (15) 0.39629 (17) 0.51813 (14) 0.0298 (4)
H2 0.1605 0.4686 0.4766 0.036*
C3 0.16580 (15) 0.26911 (17) 0.46354 (13) 0.0286 (4)
H3 0.1770 0.2538 0.3848 0.034*
C4 0.15828 (15) 0.16335 (16) 0.52411 (13) 0.0292 (4)
H4 0.1623 0.0754 0.4863 0.035*
C5 0.14493 (15) 0.18588 (15) 0.63921 (13) 0.0267 (4)
H5 0.1411 0.1133 0.6803 0.032*
C6 0.13704 (14) 0.31449 (15) 0.69539 (12) 0.0216 (3)
C7 0.12841 (16) 0.33178 (15) 0.82319 (12) 0.0254 (4)
H7 0.0469 0.2731 0.8372 0.030*
C8 0.25897 (15) 0.28997 (15) 0.88646 (12) 0.0233 (3)
C9 0.38754 (16) 0.36001 (17) 0.88849 (13) 0.0309 (4)
H9 0.3937 0.4374 0.8534 0.037*
C10 0.50688 (16) 0.31767 (18) 0.94139 (13) 0.0352 (4)
H10 0.5947 0.3656 0.9421 0.042*
C11 0.49818 (16) 0.20569 (17) 0.99316 (13) 0.0324 (4)
H11 0.5800 0.1768 1.0296 0.039*
C12 0.37035 (17) 0.13574 (16) 0.99191 (13) 0.0309 (4)
H12 0.3645 0.0585 1.0272 0.037*
C13 0.25053 (16) 0.17819 (15) 0.93923 (12) 0.0259 (4)
H13 0.1627 0.1306 0.9393 0.031*
C14 0.10830 (15) 0.57794 (17) 0.90672 (13) 0.0262 (4)
C15 0.25922 (15) 0.57519 (16) 0.25156 (13) 0.0269 (4)
H15 0.1838 0.6219 0.2249 0.032*
C16 0.26212 (16) 0.44037 (16) 0.21331 (13) 0.0305 (4)
H16 0.1888 0.3949 0.1607 0.037*
C17 0.37235 (16) 0.37218 (16) 0.25209 (13) 0.0284 (4)
H17 0.3748 0.2801 0.2256 0.034*
C18 0.47868 (16) 0.43822 (15) 0.32921 (13) 0.0260 (4)
H18 0.5539 0.3914 0.3560 0.031*
C19 0.47557 (15) 0.57276 (15) 0.36751 (12) 0.0241 (3)
H19 0.5486 0.6178 0.4206 0.029*
C20 0.36602 (15) 0.64199 (14) 0.32856 (12) 0.0208 (3)
C21 0.37093 (15) 0.79000 (14) 0.37246 (12) 0.0242 (4)
H21 0.4669 0.8293 0.3656 0.029*
C22 0.34411 (15) 0.81973 (14) 0.49715 (13) 0.0215 (3)
C23 0.45057 (16) 0.87830 (14) 0.57871 (13) 0.0249 (4)
H23 0.5404 0.9000 0.5567 0.030*
C24 0.42671 (16) 0.90538 (15) 0.69248 (13) 0.0280 (4)
H24 0.4997 0.9462 0.7478 0.034*
C25 0.29602 (16) 0.87249 (15) 0.72478 (13) 0.0277 (4)
H25 0.2791 0.8911 0.8022 0.033*
C26 0.19007 (16) 0.81236 (15) 0.64359 (13) 0.0279 (4)
H26 0.1009 0.7890 0.6659 0.034*
C27 0.21326 (15) 0.78614 (15) 0.53047 (13) 0.0249 (4)
H27 0.1401 0.7452 0.4754 0.030*
C28 0.20928 (15) 0.92584 (15) 0.25600 (12) 0.0226 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0286 (2) 0.0308 (3) 0.0386 (3) 0.00210 (18) 0.00829 (19) −0.0008 (2)
S2 0.0346 (2) 0.0281 (2) 0.0330 (3) 0.00572 (18) −0.00353 (19) 0.0080 (2)
N1 0.0422 (9) 0.0355 (9) 0.0344 (9) 0.0162 (7) 0.0031 (7) −0.0012 (7)
N2 0.0481 (9) 0.0309 (8) 0.0290 (8) 0.0109 (7) 0.0020 (7) 0.0090 (7)
C1 0.0235 (8) 0.0244 (9) 0.0313 (10) 0.0030 (7) 0.0002 (7) 0.0029 (8)
C2 0.0246 (9) 0.0332 (10) 0.0326 (10) −0.0012 (7) −0.0005 (7) 0.0120 (8)
C3 0.0204 (8) 0.0427 (11) 0.0220 (9) −0.0013 (7) 0.0023 (7) 0.0047 (8)
C4 0.0292 (9) 0.0283 (9) 0.0285 (10) 0.0042 (7) 0.0036 (7) −0.0023 (8)
C5 0.0292 (9) 0.0250 (9) 0.0271 (9) 0.0066 (7) 0.0025 (7) 0.0064 (8)
C6 0.0167 (8) 0.0251 (9) 0.0228 (9) 0.0050 (6) 0.0004 (6) 0.0031 (7)
C7 0.0245 (8) 0.0270 (9) 0.0247 (9) 0.0053 (7) 0.0034 (7) 0.0020 (7)
C8 0.0232 (8) 0.0298 (9) 0.0163 (8) 0.0047 (7) 0.0023 (6) 0.0006 (7)
C9 0.0312 (9) 0.0410 (11) 0.0218 (9) −0.0020 (8) 0.0031 (7) 0.0106 (8)
C10 0.0230 (9) 0.0561 (12) 0.0264 (10) −0.0036 (8) 0.0018 (7) 0.0096 (9)
C11 0.0275 (9) 0.0463 (12) 0.0230 (9) 0.0102 (8) −0.0007 (7) 0.0032 (8)
C12 0.0380 (10) 0.0300 (10) 0.0250 (9) 0.0085 (8) 0.0008 (8) 0.0045 (8)
C13 0.0253 (9) 0.0283 (9) 0.0225 (9) 0.0002 (7) 0.0027 (7) −0.0003 (7)
C14 0.0200 (8) 0.0382 (11) 0.0218 (9) 0.0081 (7) 0.0047 (6) 0.0052 (8)
C15 0.0214 (8) 0.0314 (10) 0.0277 (9) 0.0040 (7) 0.0001 (7) 0.0048 (8)
C16 0.0281 (9) 0.0335 (10) 0.0259 (9) −0.0053 (7) −0.0013 (7) −0.0030 (8)
C17 0.0340 (10) 0.0224 (9) 0.0289 (10) 0.0028 (7) 0.0084 (8) 0.0006 (8)
C18 0.0254 (9) 0.0264 (9) 0.0277 (9) 0.0076 (7) 0.0042 (7) 0.0057 (8)
C19 0.0210 (8) 0.0278 (9) 0.0225 (9) 0.0008 (6) 0.0004 (6) 0.0023 (7)
C20 0.0204 (8) 0.0226 (8) 0.0201 (8) 0.0015 (6) 0.0045 (6) 0.0043 (7)
C21 0.0235 (8) 0.0235 (9) 0.0271 (9) 0.0035 (7) 0.0026 (7) 0.0084 (7)
C22 0.0252 (8) 0.0152 (8) 0.0253 (9) 0.0055 (6) 0.0020 (7) 0.0051 (7)
C23 0.0231 (8) 0.0196 (8) 0.0324 (10) −0.0002 (6) 0.0011 (7) 0.0071 (7)
C24 0.0311 (9) 0.0229 (9) 0.0278 (10) −0.0020 (7) −0.0067 (7) 0.0044 (7)
C25 0.0352 (10) 0.0242 (9) 0.0243 (9) 0.0071 (7) 0.0035 (7) 0.0032 (7)
C26 0.0258 (9) 0.0276 (9) 0.0309 (10) 0.0054 (7) 0.0046 (7) 0.0039 (8)
C27 0.0216 (8) 0.0256 (9) 0.0261 (9) 0.0026 (7) −0.0016 (7) 0.0013 (7)
C28 0.0255 (8) 0.0212 (8) 0.0203 (9) −0.0005 (6) 0.0029 (6) 0.0015 (7)

Geometric parameters (Å, °)

S1—C14 1.5947 (19) C12—C13 1.388 (2)
S2—C28 1.5893 (16) C12—H12 0.9500
N1—C14 1.164 (2) C13—H13 0.9500
N1—C7 1.441 (2) C15—C20 1.388 (2)
N2—C28 1.1626 (18) C15—C16 1.389 (2)
N2—C21 1.4473 (19) C15—H15 0.9500
C1—C6 1.387 (2) C16—C17 1.388 (2)
C1—C2 1.393 (2) C16—H16 0.9500
C1—H1 0.9500 C17—C18 1.383 (2)
C2—C3 1.378 (2) C17—H17 0.9500
C2—H2 0.9500 C18—C19 1.387 (2)
C3—C4 1.390 (2) C18—H18 0.9500
C3—H3 0.9500 C19—C20 1.390 (2)
C4—C5 1.383 (2) C19—H19 0.9500
C4—H4 0.9500 C20—C21 1.523 (2)
C5—C6 1.395 (2) C21—C22 1.528 (2)
C5—H5 0.9500 C21—H21 1.0000
C6—C7 1.525 (2) C22—C23 1.389 (2)
C7—C8 1.525 (2) C22—C27 1.3949 (19)
C7—H7 1.0000 C23—C24 1.393 (2)
C8—C13 1.387 (2) C23—H23 0.9500
C8—C9 1.388 (2) C24—C25 1.387 (2)
C9—C10 1.385 (2) C24—H24 0.9500
C9—H9 0.9500 C25—C26 1.388 (2)
C10—C11 1.381 (2) C25—H25 0.9500
C10—H10 0.9500 C26—C27 1.383 (2)
C11—C12 1.383 (2) C26—H26 0.9500
C11—H11 0.9500 C27—H27 0.9500
C14—N1—C7 168.64 (16) N1—C14—S1 177.42 (15)
C28—N2—C21 168.05 (17) C20—C15—C16 120.28 (14)
C6—C1—C2 120.40 (15) C20—C15—H15 119.9
C6—C1—H1 119.8 C16—C15—H15 119.9
C2—C1—H1 119.8 C17—C16—C15 119.89 (15)
C3—C2—C1 120.23 (15) C17—C16—H16 120.1
C3—C2—H2 119.9 C15—C16—H16 120.1
C1—C2—H2 119.9 C18—C17—C16 120.02 (15)
C2—C3—C4 119.74 (15) C18—C17—H17 120.0
C2—C3—H3 120.1 C16—C17—H17 120.0
C4—C3—H3 120.1 C17—C18—C19 120.05 (14)
C5—C4—C3 120.16 (15) C17—C18—H18 120.0
C5—C4—H4 119.9 C19—C18—H18 120.0
C3—C4—H4 119.9 C18—C19—C20 120.31 (15)
C4—C5—C6 120.48 (15) C18—C19—H19 119.8
C4—C5—H5 119.8 C20—C19—H19 119.8
C6—C5—H5 119.8 C15—C20—C19 119.45 (15)
C1—C6—C5 118.97 (14) C15—C20—C21 123.10 (14)
C1—C6—C7 123.65 (14) C19—C20—C21 117.44 (14)
C5—C6—C7 117.33 (13) N2—C21—C20 111.07 (13)
N1—C7—C6 111.17 (13) N2—C21—C22 109.58 (12)
N1—C7—C8 110.31 (13) C20—C21—C22 112.88 (12)
C6—C7—C8 111.92 (12) N2—C21—H21 107.7
N1—C7—H7 107.8 C20—C21—H21 107.7
C6—C7—H7 107.8 C22—C21—H21 107.7
C8—C7—H7 107.8 C23—C22—C27 119.35 (14)
C13—C8—C9 119.46 (14) C23—C22—C21 120.30 (14)
C13—C8—C7 119.84 (14) C27—C22—C21 120.33 (14)
C9—C8—C7 120.67 (14) C22—C23—C24 120.52 (14)
C10—C9—C8 120.35 (16) C22—C23—H23 119.7
C10—C9—H9 119.8 C24—C23—H23 119.7
C8—C9—H9 119.8 C25—C24—C23 119.76 (15)
C11—C10—C9 120.00 (16) C25—C24—H24 120.1
C11—C10—H10 120.0 C23—C24—H24 120.1
C9—C10—H10 120.0 C24—C25—C26 119.79 (15)
C10—C11—C12 119.96 (15) C24—C25—H25 120.1
C10—C11—H11 120.0 C26—C25—H25 120.1
C12—C11—H11 120.0 C27—C26—C25 120.56 (15)
C11—C12—C13 120.14 (16) C27—C26—H26 119.7
C11—C12—H12 119.9 C25—C26—H26 119.7
C13—C12—H12 119.9 C26—C27—C22 120.02 (15)
C8—C13—C12 120.07 (15) C26—C27—H27 120.0
C8—C13—H13 120.0 C22—C27—H27 120.0
C12—C13—H13 120.0 N2—C28—S2 178.13 (15)
C6—C1—C2—C3 −0.1 (2) C20—C15—C16—C17 −0.1 (2)
C1—C2—C3—C4 1.0 (2) C15—C16—C17—C18 0.4 (2)
C2—C3—C4—C5 −1.4 (2) C16—C17—C18—C19 −0.3 (2)
C3—C4—C5—C6 0.8 (2) C17—C18—C19—C20 −0.1 (2)
C2—C1—C6—C5 −0.4 (2) C16—C15—C20—C19 −0.3 (2)
C2—C1—C6—C7 177.04 (14) C16—C15—C20—C21 178.89 (13)
C4—C5—C6—C1 0.1 (2) C18—C19—C20—C15 0.4 (2)
C4—C5—C6—C7 −177.57 (13) C18—C19—C20—C21 −178.82 (12)
C14—N1—C7—C6 −94.4 (8) C28—N2—C21—C20 −153.8 (7)
C14—N1—C7—C8 30.4 (8) C28—N2—C21—C22 80.8 (7)
C1—C6—C7—N1 9.4 (2) C15—C20—C21—N2 −13.98 (19)
C5—C6—C7—N1 −173.10 (13) C19—C20—C21—N2 165.23 (12)
C1—C6—C7—C8 −114.46 (16) C15—C20—C21—C22 109.54 (16)
C5—C6—C7—C8 63.05 (18) C19—C20—C21—C22 −71.24 (17)
N1—C7—C8—C13 123.86 (15) N2—C21—C22—C23 −123.47 (15)
C6—C7—C8—C13 −111.81 (15) C20—C21—C22—C23 112.18 (15)
N1—C7—C8—C9 −58.43 (18) N2—C21—C22—C27 57.70 (18)
C6—C7—C8—C9 65.90 (19) C20—C21—C22—C27 −66.65 (17)
C13—C8—C9—C10 0.9 (2) C27—C22—C23—C24 −1.0 (2)
C7—C8—C9—C10 −176.82 (14) C21—C22—C23—C24 −179.89 (13)
C8—C9—C10—C11 −0.4 (2) C22—C23—C24—C25 0.6 (2)
C9—C10—C11—C12 0.1 (2) C23—C24—C25—C26 0.2 (2)
C10—C11—C12—C13 −0.3 (2) C24—C25—C26—C27 −0.7 (2)
C9—C8—C13—C12 −1.1 (2) C25—C26—C27—C22 0.2 (2)
C7—C8—C13—C12 176.66 (13) C23—C22—C27—C26 0.6 (2)
C11—C12—C13—C8 0.8 (2) C21—C22—C27—C26 179.47 (13)
C7—N1—C14—S1 −176 (100) C21—N2—C28—S2 −168 (4)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB6596).

References

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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 datablock(s) global, I. DOI: 10.1107/S1600536812000888/hb6596sup1.cif

e-68-0o388-sup1.cif (22.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812000888/hb6596Isup2.hkl

e-68-0o388-Isup2.hkl (265.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812000888/hb6596Isup3.cml

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

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