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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 6;64(Pt 1):o157. doi: 10.1107/S1600536807063544

N-(5-Chloro-3-methyl-1-phenyl-1H-pyrazol-4-ylcarbon­yl)-N′-(2,6-dimethyl­phen­yl)thio­urea

Hai-Tang Du a,*, Hai-Jun Du b, Ming Lu c, Li-Li Sun d
PMCID: PMC2915225  PMID: 21200722

Abstract

In the title compound, C20H19ClN4OS, the pyrazole ring makes dihedral angles of 89.2 (4) and 46.4 (4)° with the phenyl and substituted benzene rings, respectively; these two six-membered rings are twisted by 52.1 (4)° with respect to each other. There are intra­molecular hydrogen bonds of types N—H⋯O and N—H⋯Cl.

Related literature

For related literature, see: Du et al. (2007); Saeed & Flörke (2007); Wang et al. (2007).graphic file with name e-64-0o157-scheme1.jpg

Experimental

Crystal data

  • C20H19ClN4OS

  • M r = 398.90

  • Monoclinic, Inline graphic

  • a = 12.0749 (12) Å

  • b = 7.6932 (8) Å

  • c = 21.090 (2) Å

  • β = 103.071 (4)°

  • V = 1908.4 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.33 mm−1

  • T = 113 (2) K

  • 0.32 × 0.18 × 0.16 mm

Data collection

  • Rigaku Saturn diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005) T min = 0.902, T max = 0.950

  • 23102 measured reflections

  • 4554 independent reflections

  • 4164 reflections with I > 2σ(I)

  • R int = 0.041

Refinement

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.090

  • S = 1.07

  • 4554 reflections

  • 256 parameters

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

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.27 e Å−3

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: CrystalStructure (Rigaku/MSC, 2005); software used to prepare material for publication: CrystalStructure.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536807063544/pv2049sup1.cif

e-64-0o157-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807063544/pv2049Isup2.hkl

e-64-0o157-Isup2.hkl (223.1KB, 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
N1—H1⋯O1 0.87 (2) 1.97 (2) 2.6744 (15) 137 (2)
N2—H2⋯Cl1 0.82 (2) 2.41 (2) 3.1175 (12) 145 (2)

Acknowledgments

The authors thank Guiyang College (No. 2007012) for financial support.

supplementary crystallographic information

Comment

In the structure of the title compound, (I), the pyrazole ring makes dihedral angles of 89.2 (4) and 46.4 (4)°, with the phenyl rings, C2—C7 and C15—C20, respectively, which are twisted by 52.1 (4)° with respect to each other (Fig. 1). However in a similar structure, N-(5-chloro-3-methyl-1-phenyl pyrazole-4-ylcarbonyl)-N' -(4-methphenyl)thiourea (Du et al., 2007), the corresponding phenyl rings from dihedral angles of 74.3 (3) and 2.9 (3)°, respectively, with the central pyrazole system and the dihedral angle between the phenyl rings is 71.6 (3)°. All the bond lengths and angles are in the normal range, corresponding to the related references (Du et al., 2007; Saeed & Flörke, 2007; Wang et al., 2007). The structure is stabilized by N—H···O and N—H···Cl intramolcular hydrogen bonds; details of hydrogen-bonding geometry have been given in the Table.

Experimental

Powdered ammonium thiocyanate (1.14 g, 15 mmol), 5-chloro-3-methyl-1-phenyl-pyrazole-4-carbonyl chloride (2.54 g, 10 mmol), polyethylene glycol-400 (0.5 ml) and acetone (25 ml) were placed in a dried round-bottomed flask containing a magnetic stirrer bar and stirred at room temperature for 1 hr, then 2,6-dimethylbenzenamine (1.15 g, 9.5 mmol) was added, and the mixture was stirred for 5 hr. The mixture was poured into water (20 ml). The resulting solid was filtered, dried and recrystallized from N,N-dimethylformamide-ethanol (1:1, v/v) to yield single crystals of (I) by slow evaporation at room temperature.

Refinement

The H-atoms bonded to N-atoms were located from difference map and were allowed to refine freely. All other H atoms were positioned geometrically and included in the refinements using a riding model, with C—H = 0.95 and 0.98 Å and Uiso(H) = 1.2 and 1.5 times Ueq(C), respectively, for the aromatic and methyl type H-atoms.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) with the atomic numbering scheme, showing displacement ellipsoids at 50% probability level. Intramolcular hydrogen bonds have been represented by dashed lines.

Crystal data

C20H19ClN4OS F000 = 832
Mr = 398.90 Dx = 1.388 Mg m3
Monoclinic, P21/n Melting point: 459 K
Hall symbol: -P 2yn Mo Kα radiation λ = 0.71070 Å
a = 12.0749 (12) Å Cell parameters from 5929 reflections
b = 7.6932 (8) Å θ = 1.8–27.9º
c = 21.090 (2) Å µ = 0.33 mm1
β = 103.071 (4)º T = 113 (2) K
V = 1908.4 (3) Å3 Prism, colorless
Z = 4 0.32 × 0.18 × 0.16 mm

Data collection

Rigaku Saturn diffractometer 4554 independent reflections
Radiation source: rotating anode 4164 reflections with I > 2σ(I)
Monochromator: confocal Rint = 0.041
Detector resolution: 7.31 pixels mm-1 θmax = 27.9º
T = 113(2) K θmin = 1.8º
ω scans h = −15→15
Absorption correction: multi-scan(CrystalClear; Rigaku/MSC, 2005) k = −10→10
Tmin = 0.902, Tmax = 0.950 l = −26→27
23102 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: geom/difmap
R[F2 > 2σ(F2)] = 0.036 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.090   w = 1/[σ2(Fo2) + (0.0402P)2 + 0.794P] where P = (Fo2 + 2Fc2)/3
S = 1.07 (Δ/σ)max = 0.001
4554 reflections Δρmax = 0.31 e Å3
256 parameters Δρmin = −0.27 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

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
Cl1 0.43026 (3) 0.10904 (5) 0.202263 (15) 0.02133 (10)
S1 0.79209 (3) −0.08648 (5) 0.266243 (16) 0.02236 (10)
O1 0.63163 (9) 0.16452 (16) 0.41897 (5) 0.0287 (3)
N1 0.81514 (9) 0.02276 (15) 0.38858 (5) 0.0172 (2)
N2 0.64393 (10) 0.08216 (15) 0.31685 (6) 0.0169 (2)
N3 0.28650 (10) 0.27287 (16) 0.33684 (5) 0.0194 (2)
N4 0.29269 (9) 0.22644 (15) 0.27493 (5) 0.0165 (2)
C1 0.75248 (11) 0.00996 (17) 0.32786 (6) 0.0160 (3)
C2 0.92637 (11) −0.05169 (18) 0.40858 (6) 0.0162 (3)
C3 1.02093 (11) 0.05457 (18) 0.41050 (6) 0.0180 (3)
C4 1.12834 (11) −0.0181 (2) 0.43418 (7) 0.0210 (3)
H4 1.1942 0.0515 0.4367 0.025*
C5 1.14034 (12) −0.1897 (2) 0.45402 (6) 0.0211 (3)
H5 1.2140 −0.2368 0.4704 0.025*
C6 1.04501 (12) −0.29323 (19) 0.45006 (6) 0.0198 (3)
H6 1.0541 −0.4117 0.4630 0.024*
C7 0.93592 (11) −0.22569 (18) 0.42738 (6) 0.0173 (3)
C8 1.00655 (13) 0.23944 (19) 0.38786 (7) 0.0247 (3)
H8A 0.9586 0.2434 0.3437 0.037*
H8B 1.0812 0.2896 0.3879 0.037*
H8C 0.9704 0.3063 0.4172 0.037*
C9 0.83187 (12) −0.3363 (2) 0.42329 (8) 0.0259 (3)
H9A 0.7848 −0.2863 0.4509 0.039*
H9B 0.8549 −0.4543 0.4382 0.039*
H9C 0.7882 −0.3405 0.3781 0.039*
C10 0.58681 (11) 0.14840 (18) 0.36088 (6) 0.0176 (3)
C11 0.46730 (11) 0.19453 (18) 0.33493 (6) 0.0164 (3)
C12 0.39116 (11) 0.25472 (19) 0.37263 (6) 0.0187 (3)
C13 0.39920 (11) 0.17882 (17) 0.27273 (6) 0.0161 (3)
C14 0.41480 (13) 0.2956 (2) 0.44358 (7) 0.0267 (3)
H14A 0.3477 0.3503 0.4539 0.040*
H14B 0.4796 0.3753 0.4547 0.040*
H14C 0.4326 0.1880 0.4687 0.040*
C15 0.19141 (11) 0.22612 (18) 0.22397 (6) 0.0164 (3)
C16 0.09328 (11) 0.15251 (19) 0.23588 (7) 0.0196 (3)
H16 0.0933 0.1027 0.2771 0.024*
C17 −0.00513 (12) 0.1527 (2) 0.18663 (7) 0.0236 (3)
H17 −0.0735 0.1053 0.1944 0.028*
C18 −0.00365 (12) 0.2219 (2) 0.12628 (7) 0.0247 (3)
H18 −0.0706 0.2192 0.0924 0.030*
C19 0.09488 (12) 0.2950 (2) 0.11495 (7) 0.0233 (3)
H19 0.0954 0.3421 0.0734 0.028*
C20 0.19313 (11) 0.29973 (18) 0.16438 (7) 0.0191 (3)
H20 0.2604 0.3527 0.1573 0.023*
H1 0.7828 (15) 0.073 (2) 0.4168 (9) 0.024 (4)*
H2 0.6098 (16) 0.072 (2) 0.2787 (10) 0.034 (5)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.01647 (16) 0.0336 (2) 0.01365 (15) 0.00392 (13) 0.00286 (12) −0.00437 (12)
S1 0.02202 (18) 0.0291 (2) 0.01609 (17) 0.00740 (14) 0.00459 (13) −0.00227 (13)
O1 0.0192 (5) 0.0482 (7) 0.0168 (5) 0.0090 (5) 0.0000 (4) −0.0079 (5)
N1 0.0155 (5) 0.0217 (6) 0.0142 (5) 0.0046 (5) 0.0029 (4) −0.0010 (4)
N2 0.0141 (5) 0.0235 (6) 0.0124 (5) 0.0036 (4) 0.0012 (4) 0.0006 (4)
N3 0.0177 (6) 0.0266 (6) 0.0141 (5) 0.0026 (5) 0.0043 (4) −0.0020 (5)
N4 0.0146 (5) 0.0226 (6) 0.0121 (5) 0.0013 (4) 0.0024 (4) −0.0007 (4)
C1 0.0161 (6) 0.0156 (6) 0.0165 (6) 0.0012 (5) 0.0043 (5) 0.0025 (5)
C2 0.0136 (6) 0.0222 (7) 0.0127 (6) 0.0033 (5) 0.0029 (5) −0.0007 (5)
C3 0.0191 (6) 0.0215 (7) 0.0143 (6) 0.0007 (5) 0.0056 (5) −0.0028 (5)
C4 0.0154 (6) 0.0297 (8) 0.0183 (6) −0.0023 (6) 0.0048 (5) −0.0065 (6)
C5 0.0148 (6) 0.0325 (8) 0.0152 (6) 0.0063 (6) 0.0014 (5) −0.0037 (5)
C6 0.0211 (7) 0.0235 (7) 0.0144 (6) 0.0060 (5) 0.0033 (5) 0.0016 (5)
C7 0.0163 (6) 0.0218 (7) 0.0138 (6) 0.0026 (5) 0.0032 (5) −0.0001 (5)
C8 0.0290 (8) 0.0213 (7) 0.0265 (7) −0.0014 (6) 0.0116 (6) −0.0007 (6)
C9 0.0215 (7) 0.0243 (8) 0.0306 (8) −0.0002 (6) 0.0033 (6) 0.0075 (6)
C10 0.0153 (6) 0.0199 (6) 0.0170 (6) 0.0003 (5) 0.0025 (5) −0.0007 (5)
C11 0.0151 (6) 0.0191 (7) 0.0145 (6) 0.0011 (5) 0.0024 (5) −0.0004 (5)
C12 0.0174 (6) 0.0227 (7) 0.0160 (6) 0.0022 (5) 0.0037 (5) −0.0013 (5)
C13 0.0158 (6) 0.0185 (6) 0.0145 (6) 0.0011 (5) 0.0046 (5) −0.0001 (5)
C14 0.0216 (7) 0.0412 (9) 0.0168 (7) 0.0047 (6) 0.0035 (5) −0.0062 (6)
C15 0.0140 (6) 0.0189 (6) 0.0155 (6) 0.0021 (5) 0.0014 (5) −0.0026 (5)
C16 0.0177 (6) 0.0236 (7) 0.0183 (6) 0.0008 (5) 0.0056 (5) 0.0005 (5)
C17 0.0143 (6) 0.0296 (8) 0.0270 (7) −0.0014 (6) 0.0047 (6) −0.0025 (6)
C18 0.0169 (7) 0.0328 (8) 0.0218 (7) 0.0023 (6) −0.0013 (5) −0.0021 (6)
C19 0.0209 (7) 0.0295 (8) 0.0178 (6) 0.0033 (6) 0.0012 (5) 0.0032 (6)
C20 0.0155 (6) 0.0224 (7) 0.0191 (6) 0.0004 (5) 0.0031 (5) 0.0014 (5)

Geometric parameters (Å, °)

Cl1—C13 1.6998 (13) C8—H8A 0.9800
S1—C1 1.6581 (13) C8—H8B 0.9800
O1—C10 1.2284 (16) C8—H8C 0.9800
N1—C1 1.3355 (17) C9—H9A 0.9800
N1—C2 1.4331 (16) C9—H9B 0.9800
N1—H1 0.87 (2) C9—H9C 0.9800
N2—C10 1.3738 (17) C10—C11 1.4665 (18)
N2—C1 1.3939 (17) C11—C13 1.3869 (18)
N2—H2 0.82 (2) C11—C12 1.4222 (18)
N3—C12 1.3247 (17) C12—C14 1.4920 (18)
N3—N4 1.3719 (15) C14—H14A 0.9800
N4—C13 1.3482 (17) C14—H14B 0.9800
N4—C15 1.4339 (16) C14—H14C 0.9800
C2—C7 1.3935 (19) C15—C20 1.3828 (19)
C2—C3 1.3974 (19) C15—C16 1.3865 (19)
C3—C4 1.3968 (19) C16—C17 1.3902 (19)
C3—C8 1.498 (2) C16—H16 0.9500
C4—C5 1.383 (2) C17—C18 1.383 (2)
C4—H4 0.9500 C17—H17 0.9500
C5—C6 1.387 (2) C18—C19 1.385 (2)
C5—H5 0.9500 C18—H18 0.9500
C6—C7 1.3960 (18) C19—C20 1.3915 (19)
C6—H6 0.9500 C19—H19 0.9500
C7—C9 1.5038 (19) C20—H20 0.9500
C1—N1—C2 122.87 (11) C7—C9—H9C 109.5
C1—N1—H1 116.2 (11) H9A—C9—H9C 109.5
C2—N1—H1 120.8 (11) H9B—C9—H9C 109.5
C10—N2—C1 129.21 (11) O1—C10—N2 122.43 (12)
C10—N2—H2 118.6 (14) O1—C10—C11 121.48 (12)
C1—N2—H2 111.8 (13) N2—C10—C11 116.07 (11)
C12—N3—N4 105.34 (11) C13—C11—C12 103.72 (11)
C13—N4—N3 111.18 (10) C13—C11—C10 130.91 (12)
C13—N4—C15 129.22 (11) C12—C11—C10 125.17 (12)
N3—N4—C15 119.54 (10) N3—C12—C11 111.70 (12)
N1—C1—N2 115.97 (12) N3—C12—C14 119.38 (12)
N1—C1—S1 125.67 (10) C11—C12—C14 128.91 (12)
N2—C1—S1 118.35 (10) N4—C13—C11 108.05 (11)
C7—C2—C3 122.63 (12) N4—C13—Cl1 121.12 (10)
C7—C2—N1 118.65 (12) C11—C13—Cl1 130.81 (11)
C3—C2—N1 118.69 (12) C12—C14—H14A 109.5
C4—C3—C2 117.57 (13) C12—C14—H14B 109.5
C4—C3—C8 121.68 (13) H14A—C14—H14B 109.5
C2—C3—C8 120.75 (12) C12—C14—H14C 109.5
C5—C4—C3 121.03 (13) H14A—C14—H14C 109.5
C5—C4—H4 119.5 H14B—C14—H14C 109.5
C3—C4—H4 119.5 C20—C15—C16 121.40 (12)
C4—C5—C6 120.10 (13) C20—C15—N4 119.66 (12)
C4—C5—H5 119.9 C16—C15—N4 118.94 (12)
C6—C5—H5 119.9 C15—C16—C17 119.03 (13)
C5—C6—C7 120.86 (13) C15—C16—H16 120.5
C5—C6—H6 119.6 C17—C16—H16 120.5
C7—C6—H6 119.6 C18—C17—C16 120.08 (13)
C2—C7—C6 117.78 (13) C18—C17—H17 120.0
C2—C7—C9 120.86 (12) C16—C17—H17 120.0
C6—C7—C9 121.36 (13) C17—C18—C19 120.36 (13)
C3—C8—H8A 109.5 C17—C18—H18 119.8
C3—C8—H8B 109.5 C19—C18—H18 119.8
H8A—C8—H8B 109.5 C18—C19—C20 120.09 (13)
C3—C8—H8C 109.5 C18—C19—H19 120.0
H8A—C8—H8C 109.5 C20—C19—H19 120.0
H8B—C8—H8C 109.5 C15—C20—C19 119.00 (13)
C7—C9—H9A 109.5 C15—C20—H20 120.5
C7—C9—H9B 109.5 C19—C20—H20 120.5
H9A—C9—H9B 109.5
C12—N3—N4—C13 0.60 (15) N2—C10—C11—C12 175.91 (13)
C12—N3—N4—C15 177.88 (12) N4—N3—C12—C11 −0.58 (16)
C2—N1—C1—N2 177.06 (12) N4—N3—C12—C14 179.86 (13)
C2—N1—C1—S1 −1.7 (2) C13—C11—C12—N3 0.36 (16)
C10—N2—C1—N1 −7.9 (2) C10—C11—C12—N3 −174.98 (13)
C10—N2—C1—S1 170.98 (12) C13—C11—C12—C14 179.87 (15)
C1—N1—C2—C7 −84.89 (16) C10—C11—C12—C14 4.5 (2)
C1—N1—C2—C3 97.20 (16) N3—N4—C13—C11 −0.38 (16)
C7—C2—C3—C4 −1.91 (19) C15—N4—C13—C11 −177.33 (13)
N1—C2—C3—C4 175.92 (11) N3—N4—C13—Cl1 178.12 (9)
C7—C2—C3—C8 178.10 (12) C15—N4—C13—Cl1 1.2 (2)
N1—C2—C3—C8 −4.07 (19) C12—C11—C13—N4 0.02 (15)
C2—C3—C4—C5 0.97 (19) C10—C11—C13—N4 174.98 (14)
C8—C3—C4—C5 −179.04 (12) C12—C11—C13—Cl1 −178.29 (11)
C3—C4—C5—C6 0.6 (2) C10—C11—C13—Cl1 −3.3 (2)
C4—C5—C6—C7 −1.3 (2) C13—N4—C15—C20 −48.8 (2)
C3—C2—C7—C6 1.24 (19) N3—N4—C15—C20 134.47 (14)
N1—C2—C7—C6 −176.58 (11) C13—N4—C15—C16 131.62 (15)
C3—C2—C7—C9 −178.78 (13) N3—N4—C15—C16 −45.11 (18)
N1—C2—C7—C9 3.40 (19) C20—C15—C16—C17 0.2 (2)
C5—C6—C7—C2 0.39 (19) N4—C15—C16—C17 179.73 (12)
C5—C6—C7—C9 −179.59 (13) C15—C16—C17—C18 1.5 (2)
C1—N2—C10—O1 6.0 (2) C16—C17—C18—C19 −1.6 (2)
C1—N2—C10—C11 −172.25 (13) C17—C18—C19—C20 −0.1 (2)
O1—C10—C11—C13 −176.38 (15) C16—C15—C20—C19 −1.8 (2)
N2—C10—C11—C13 1.9 (2) N4—C15—C20—C19 178.60 (12)
O1—C10—C11—C12 −2.4 (2) C18—C19—C20—C15 1.8 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O1 0.87 (2) 1.97 (2) 2.6744 (15) 137 (2)
N2—H2···Cl1 0.82 (2) 2.41 (2) 3.1175 (12) 145 (2)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2049).

References

  1. Du, H.-T., Lu, M., Zhou, W.-Y. & Sun, L.-L. (2007). Acta Cryst. E63, o4287.
  2. Rigaku/MSC. (2005). CrystalClear and CrystalStructure Rigaku/MSC, The Woodlands, Texas, USA.
  3. Saeed, A. & Flörke, U. (2007). Acta Cryst. E63, o3695.
  4. Sheldrick, G. M. (1997). SHELXS97 and SHELXL97 University of Göttingen, Germany.
  5. Wang, J., Tian, L. & Liu, S.-Y. (2007). Acta Cryst. E63, o3667.

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/S1600536807063544/pv2049sup1.cif

e-64-0o157-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807063544/pv2049Isup2.hkl

e-64-0o157-Isup2.hkl (223.1KB, 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

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