organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

3-[3-Methyl-4-(4-nitro­benzyl­­idene­amino)-5-sulfanyl­­idene-4,5-di­hydro-1H-1,2,4-triazol-1-yl]-1,3-di­phenyl­propan-1-one di­chloro­methane monosolvate

aSchool of Perfume and Aroma Technology, Shanghai Institute of Technology, Shanghai 200235, People's Republic of China, and bSchool of Chemical Engineering, University of Science and Technology Liaoning, Anshan 114051, People's Republic of China
*Correspondence e-mail: zhao_submit@yahoo.com.cn

(Received 15 August 2011; accepted 21 October 2011; online 29 October 2011)

In the title compound, C25H21N5O3S·CH2Cl2, the dichloro­methane solvent mol­ecule is disordered over four positions, with an occupancy ratio of 0.271 (3):0.3884 (18):0.298 (2):0.0424 (15). The 1,2,4-triazole ring makes dihedral angles of 47.3 (2)/87.3 (2) and 3.6 (2)° with the phenyl and nitro­phenyl rings, respectively. An intra­molecular C—H⋯S hydrogen bond results in the formation of an almost planar six-membered ring [r.m.s. derivation = 0.0051 (2) Å]. Inter­molecular C—H⋯O hydrogen bonding consolidates the structure.

Related literature

For crystal structures related to 1,2,4-triazole-5(4H)-thione, see: Al-Tamimi et al. (2010[Al-Tamimi, A.-M. S., Bari, A., Al-Omar, M. A., Alrashood, K. A. & El-Emam, A. A. (2010). Acta Cryst. E66, o1756.]); Fun et al. (2009[Fun, H.-K., Chantrapromma, S., Sujith, K. V. & Kalluraya, B. (2009). Acta Cryst. E65, o495-o496.]); Gao et al. (2011[Gao, Y., Zhang, L. & Wang, H. (2011). Acta Cryst. E67, o1794.]); Tan et al. (2010[Tan, K. W., Maah, M. J. & Ng, S. W. (2010). Acta Cryst. E66, o2224.]); Wang et al. (2011[Wang, W., Gao, Y., Xiao, Z., Yao, H. & Zhang, J. (2011). Acta Cryst. E67, o269.]); Zhao et al. (2010[Zhao, B., Liu, Z., Gao, Y., Song, B. & Deng, Q. (2010). Acta Cryst. E66, o2814.]).

[Scheme 1]

Experimental

Crystal data
  • C25H21N5O3S·CH2Cl2

  • Mr = 556.45

  • Triclinic, [P \overline 1]

  • a = 8.9880 (13) Å

  • b = 11.4440 (15) Å

  • c = 14.8604 (18) Å

  • α = 70.212 (11)°

  • β = 88.973 (13)°

  • γ = 67.020 (9)°

  • V = 1312.6 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.37 mm−1

  • T = 113 K

  • 0.26 × 0.24 × 0.20 mm

Data collection
  • Rigaku Saturn CCD diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear. Rigaku/MSC, The Woodlands, Texas, USA.]) Tmin = 0.911, Tmax = 0.931

  • 16932 measured reflections

  • 6203 independent reflections

  • 4100 reflections with I > 2σ(I)

  • Rint = 0.035

Refinement
  • R[F2 > 2σ(F2)] = 0.052

  • wR(F2) = 0.159

  • S = 1.07

  • 6203 reflections

  • 396 parameters

  • 91 restraints

  • H-atom parameters constrained

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.41 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C19—H19⋯S1 0.95 2.43 3.199 (3) 137
C18—H18B⋯O1i 0.98 2.55 3.443 (4) 152
C22—H22⋯O1ii 0.95 2.34 3.202 (3) 151
Symmetry codes: (i) x-1, y, z; (ii) -x+1, -y+1, -z.

Data collection: CrystalClear (Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear. Rigaku/MSC, The Woodlands, Texas, USA.]); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: CrystalStructure (Rigaku/MSC, 2007[Rigaku/MSC (2007). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.]).

Supporting information


Comment top

In continuation of our structural studies of derivatives of Mannich bases synthesized from amino heterocycles and aromatic aldehydes in our group (Wang et al., 2011), we present here the crystal structure of the title compound named 3-[4-(4-Nitrobenzylideneamino)-5-thioxo-3-(4-tolyl)-4,5- dihydro-1H-1,2,4-triazol-1-yl]-1,3-diphenylpropan-1-one.

The bond lengths and angles in title compound are found to have normal values comparable with those reported in related 1,2,4-triazole- 5(4H)-thione derivatives (Al-Tamimi et al., 2010; Fun et al., 2009; Tan et al., 2010; Wang et al., 2011). An intramolecular C—H···S hydrogen bond results in the formation of a planar [an r.m.s. deviation of 0.0051 (2) Å] six-membered ring (Table 1) and the maxmium deviation of 0.0088 (2) Å for atom N4. The 1,2,4-triazole ring is almost planar with an r.m.s. deviation of 0.0039 (2) Å and the maxmium deviation of 0.0061 (2) Å for atom N1. The 1,2,4-triazole ring mean plane forms the dihedral angles of 47.3 (2), 87.3 (2) and 3.6 (2)° with two phenyl rings (C1–C6 and C10–C15) and nitrophenyl ring, respectively. Two C atoms in the 1,2,4-triazole ring show distorted Csp2 hybridization states with the bond angles of 101.95 (16)° (N1—C16—N3), 130.44 (15)° (N3—C16—S1), 110.44 (18)° (N2—C17—N3) and 25.88 (19)° (N3—C17—C18), which are similar to those of similar reported triazole derivatives (Zhao et al., 2010; Gao et al., 2011).

In the crystal structure, weak intermolecular C—H···O hydrogen bonds (Table 1) are observed and consolidate the crystal structure.

Related literature top

For crystal structures related to 1,2,4-triazole-5(4H)-thione, see: Al-Tamimi et al. (2010); Fun et al. (2009); Gao et al. (2011); Tan et al. (2010); Wang et al. (2011); Zhao et al. (2010).

Experimental top

The title compound was synthesized with the reaction of 4-nitrobenzaldehyde (2.0 mmol) and 3-(4-amino-3-methyl-5-thioxo-4,5-dihydro-1H-1,2,4-triazol-1-yl)-1,3-diphenylpropan-1-one (2.0 mmol) by refluxing in ethanol. The reaction progress was monitored via TLC. The resulting precipitate was filtered off, washed with cold ethanol, dried and purified to give the target product as a colorless solid in 74% yield. Crystals of title compound suitable for single-crystal X-ray analysis were grown by slow evaporation of a solution in dichloromethanle–ethanol (1:1).

Refinement top

All H atoms were positioned geometrically and refined as riding (C—H = 0.95–1.00 Å) on their parent atoms, with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(C). One molecule of solvent dichloromethane is present in the asymmetric unit. This was refined as disordered over four positions with occupancies of 0.271 (3):0.3884 (18):0.298 (2):0.0424 (15).

Computing details top

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); 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: CrystalStructure (Rigaku/MSC, 2007).

Figures top
[Figure 1] Fig. 1. View of the molecule of (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 60% probability level. The disordered dichloromethane molecule is omitted.
[Figure 2] Fig. 2. Packing diagram of the crystal structure. The disordered dichloromethane molecule is omitted.
3-[3-Methyl-4-(4-nitrobenzylideneamino)-5-sulfanylidene-4,5-dihydro-1H- 1,2,4-triazol-1-yl]-1,3-diphenylpropan-1-one dichloromethane monosolvate top
Crystal data top
C25H21N5O3S·CH2Cl2Z = 2
Mr = 556.45F(000) = 576
Triclinic, P1Dx = 1.408 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.9880 (13) ÅCell parameters from 4632 reflections
b = 11.4440 (15) Åθ = 2.1–27.9°
c = 14.8604 (18) ŵ = 0.37 mm1
α = 70.212 (11)°T = 113 K
β = 88.973 (13)°Prism, colourless
γ = 67.020 (9)°0.26 × 0.24 × 0.20 mm
V = 1312.6 (3) Å3
Data collection top
Rigaku Saturn CCD
diffractometer
6203 independent reflections
Radiation source: rotating anode4100 reflections with I > 2σ(I)
Multilayer monochromatorRint = 0.035
Detector resolution: 14.22 pixels mm-1θmax = 27.9°, θmin = 2.1°
ϕ and ω scansh = 1111
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
k = 1515
Tmin = 0.911, Tmax = 0.931l = 1918
16932 measured reflections
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)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.159H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0904P)2]
where P = (Fo2 + 2Fc2)/3
6203 reflections(Δ/σ)max = 0.003
396 parametersΔρmax = 0.27 e Å3
91 restraintsΔρmin = 0.41 e Å3
Crystal data top
C25H21N5O3S·CH2Cl2γ = 67.020 (9)°
Mr = 556.45V = 1312.6 (3) Å3
Triclinic, P1Z = 2
a = 8.9880 (13) ÅMo Kα radiation
b = 11.4440 (15) ŵ = 0.37 mm1
c = 14.8604 (18) ÅT = 113 K
α = 70.212 (11)°0.26 × 0.24 × 0.20 mm
β = 88.973 (13)°
Data collection top
Rigaku Saturn CCD
diffractometer
6203 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
4100 reflections with I > 2σ(I)
Tmin = 0.911, Tmax = 0.931Rint = 0.035
16932 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.05291 restraints
wR(F2) = 0.159H-atom parameters constrained
S = 1.07Δρmax = 0.27 e Å3
6203 reflectionsΔρmin = 0.41 e Å3
396 parameters
Special details top

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*/UeqOcc. (<1)
S10.48389 (7)0.55051 (6)0.09792 (4)0.03327 (18)
O10.91577 (19)0.35679 (16)0.36980 (12)0.0382 (4)
O20.3675 (2)0.7421 (2)0.32320 (14)0.0570 (5)
O30.5429 (2)0.7897 (2)0.22653 (14)0.0565 (5)
N10.4215 (2)0.54864 (17)0.27759 (11)0.0220 (4)
N20.2982 (2)0.57257 (18)0.33400 (12)0.0252 (4)
N40.0767 (2)0.63610 (17)0.12001 (12)0.0253 (4)
N50.4037 (3)0.75374 (19)0.24612 (15)0.0387 (5)
C11.0752 (3)0.1110 (2)0.52278 (17)0.0316 (5)
H11.13630.13710.47300.038*
C21.1508 (3)0.0061 (2)0.60281 (18)0.0376 (6)
H21.26340.06140.60720.045*
C31.0636 (3)0.0431 (2)0.67630 (18)0.0390 (6)
H31.11690.12280.73160.047*
C40.8977 (3)0.0356 (2)0.67000 (17)0.0401 (6)
H40.83770.00970.72060.048*
C50.8204 (3)0.1531 (2)0.58855 (16)0.0320 (5)
H50.70720.20700.58350.038*
C60.9085 (2)0.1913 (2)0.51510 (15)0.0262 (4)
C70.8314 (3)0.3141 (2)0.42531 (15)0.0270 (5)
C80.6478 (2)0.3800 (2)0.40255 (15)0.0270 (5)
H8A0.59980.39760.45960.032*
H8B0.60980.31670.38880.032*
C90.5887 (2)0.5135 (2)0.31618 (14)0.0232 (4)
H90.65960.49830.26500.028*
C100.5934 (2)0.6341 (2)0.33558 (15)0.0246 (4)
C110.5370 (3)0.7600 (2)0.25927 (17)0.0331 (5)
H110.50270.76640.19700.040*
C120.5308 (3)0.8754 (3)0.2736 (2)0.0440 (6)
H120.49080.96060.22170.053*
C130.5833 (3)0.8658 (3)0.3641 (2)0.0469 (7)
H130.57850.94460.37430.056*
C140.6420 (3)0.7426 (3)0.43870 (19)0.0406 (6)
H140.67870.73620.50040.049*
C150.6480 (3)0.6268 (2)0.42456 (16)0.0284 (5)
H150.69020.54170.47660.034*
C160.3708 (2)0.56787 (19)0.18648 (14)0.0228 (4)
N30.2032 (2)0.60395 (16)0.18804 (12)0.0223 (4)
C170.1673 (2)0.6053 (2)0.27919 (14)0.0249 (4)
C180.0009 (3)0.6404 (3)0.30726 (17)0.0363 (5)
H18A0.00460.63540.37440.054*
H18B0.04120.57620.30080.054*
H18C0.07070.73290.26520.054*
C190.1070 (3)0.6337 (2)0.03578 (15)0.0275 (5)
H190.21480.61180.01950.033*
C200.0282 (3)0.6655 (2)0.03495 (15)0.0264 (5)
C210.0061 (3)0.6678 (2)0.12770 (16)0.0303 (5)
H210.11400.64930.14300.036*
C220.1174 (3)0.6972 (2)0.19751 (16)0.0318 (5)
H220.09550.69980.26080.038*
C230.2716 (3)0.7224 (2)0.17278 (15)0.0297 (5)
C240.3097 (3)0.7184 (2)0.08119 (16)0.0324 (5)
H240.41760.73520.06620.039*
C250.1863 (3)0.6893 (2)0.01263 (16)0.0311 (5)
H250.20930.68550.05070.037*
Cl10.8120 (5)1.0389 (4)0.0808 (3)0.0362 (8)0.271 (3)
Cl20.7811 (5)1.0728 (4)0.0934 (3)0.0640 (12)0.271 (3)
C260.6696 (14)1.0852 (19)0.0030 (9)0.094 (3)0.271 (3)
H26A0.58681.17940.03480.112*0.271 (3)
H26B0.61371.02290.01700.112*0.271 (3)
C270.7212 (11)0.9953 (13)0.0241 (7)0.094 (3)0.3884 (18)
H27A0.79770.90210.03050.112*0.3884 (18)
H27B0.74131.05850.03430.112*0.3884 (18)
Cl30.5337 (2)1.0078 (2)0.00310 (16)0.0435 (6)0.3884 (18)
Cl40.7722 (3)1.0250 (3)0.11800 (18)0.0621 (7)0.3884 (18)
C280.9267 (13)0.9766 (13)0.0362 (7)0.079 (4)0.298 (2)
H28A0.93290.88300.05500.095*0.298 (2)
H28B0.84101.02250.07050.095*0.298 (2)
Cl61.1012 (7)0.9588 (6)0.0885 (4)0.0887 (19)0.298 (2)
Cl50.8513 (7)1.0491 (5)0.0756 (4)0.0586 (13)0.298 (2)
Cl71.0305 (17)0.9999 (14)0.0990 (9)0.0362 (8)0.0424 (15)
Cl81.176 (3)1.000 (2)0.0685 (12)0.0362 (8)0.0424 (15)
C291.185 (7)0.908 (4)0.004 (4)0.079 (4)0.0424 (15)
H29A1.29150.88430.02900.095*0.0424 (15)
H29B1.17580.82190.03450.095*0.0424 (15)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0257 (3)0.0509 (4)0.0245 (3)0.0139 (3)0.0057 (2)0.0174 (3)
O10.0242 (8)0.0376 (9)0.0401 (9)0.0080 (7)0.0043 (7)0.0043 (8)
O20.0592 (13)0.0715 (13)0.0390 (11)0.0221 (11)0.0150 (9)0.0229 (10)
O30.0368 (11)0.0656 (13)0.0511 (12)0.0185 (10)0.0200 (9)0.0036 (10)
N10.0193 (8)0.0270 (9)0.0185 (8)0.0089 (7)0.0019 (6)0.0073 (7)
N20.0218 (8)0.0323 (9)0.0213 (8)0.0107 (7)0.0031 (7)0.0098 (8)
N40.0229 (9)0.0259 (9)0.0234 (9)0.0079 (7)0.0056 (7)0.0065 (7)
N50.0428 (13)0.0293 (10)0.0365 (12)0.0141 (9)0.0164 (10)0.0029 (9)
C10.0258 (11)0.0290 (11)0.0397 (13)0.0120 (9)0.0047 (10)0.0106 (10)
C20.0275 (12)0.0291 (12)0.0502 (15)0.0093 (10)0.0122 (11)0.0088 (11)
C30.0400 (14)0.0278 (12)0.0373 (13)0.0088 (11)0.0169 (11)0.0024 (10)
C40.0469 (15)0.0356 (13)0.0289 (12)0.0140 (12)0.0045 (11)0.0039 (11)
C50.0299 (12)0.0309 (11)0.0284 (11)0.0067 (10)0.0033 (9)0.0090 (10)
C60.0241 (10)0.0240 (10)0.0291 (11)0.0086 (9)0.0046 (9)0.0092 (9)
C70.0244 (10)0.0265 (10)0.0292 (11)0.0091 (9)0.0017 (9)0.0102 (9)
C80.0232 (10)0.0259 (10)0.0277 (11)0.0104 (9)0.0010 (8)0.0043 (9)
C90.0170 (9)0.0270 (10)0.0213 (10)0.0075 (8)0.0002 (8)0.0050 (8)
C100.0185 (9)0.0289 (11)0.0269 (10)0.0110 (8)0.0031 (8)0.0090 (9)
C110.0350 (12)0.0322 (12)0.0311 (12)0.0174 (10)0.0005 (10)0.0058 (10)
C120.0467 (15)0.0329 (13)0.0494 (16)0.0211 (12)0.0000 (12)0.0055 (12)
C130.0467 (15)0.0402 (14)0.0666 (19)0.0257 (12)0.0034 (14)0.0248 (14)
C140.0380 (13)0.0565 (16)0.0431 (14)0.0270 (12)0.0052 (11)0.0275 (13)
C150.0243 (10)0.0351 (12)0.0259 (11)0.0135 (9)0.0025 (9)0.0095 (9)
C160.0223 (10)0.0215 (10)0.0231 (10)0.0084 (8)0.0002 (8)0.0068 (8)
N30.0202 (8)0.0246 (9)0.0206 (8)0.0082 (7)0.0001 (7)0.0073 (7)
C170.0244 (10)0.0293 (11)0.0211 (10)0.0116 (9)0.0029 (8)0.0083 (9)
C180.0237 (11)0.0567 (15)0.0323 (12)0.0167 (11)0.0073 (9)0.0204 (12)
C190.0260 (11)0.0267 (11)0.0271 (11)0.0102 (9)0.0011 (9)0.0068 (9)
C200.0283 (11)0.0227 (10)0.0242 (10)0.0095 (9)0.0038 (9)0.0043 (9)
C210.0310 (11)0.0334 (11)0.0263 (11)0.0145 (10)0.0004 (9)0.0088 (9)
C220.0378 (13)0.0306 (11)0.0243 (11)0.0139 (10)0.0026 (9)0.0063 (9)
C230.0349 (12)0.0217 (10)0.0256 (11)0.0105 (9)0.0122 (9)0.0007 (9)
C240.0265 (11)0.0318 (12)0.0346 (12)0.0101 (10)0.0023 (9)0.0088 (10)
C250.0299 (11)0.0339 (12)0.0254 (11)0.0113 (10)0.0012 (9)0.0078 (10)
Cl10.0368 (10)0.0373 (10)0.0345 (9)0.0143 (6)0.0046 (6)0.0140 (6)
Cl20.0677 (15)0.0600 (14)0.0678 (15)0.0239 (10)0.0039 (9)0.0294 (10)
C260.094 (3)0.093 (3)0.093 (3)0.0377 (14)0.0128 (9)0.0339 (13)
C270.094 (3)0.093 (3)0.093 (3)0.0377 (14)0.0128 (9)0.0339 (13)
Cl30.0459 (10)0.0446 (8)0.0421 (7)0.0168 (7)0.0075 (8)0.0201 (6)
Cl40.0617 (10)0.0766 (11)0.0486 (10)0.0279 (8)0.0057 (7)0.0234 (8)
C280.079 (4)0.079 (4)0.079 (4)0.0324 (16)0.0104 (9)0.0286 (15)
Cl60.089 (2)0.088 (2)0.090 (2)0.0372 (12)0.0078 (10)0.0314 (11)
Cl50.0574 (16)0.0577 (15)0.0607 (15)0.0229 (10)0.0094 (10)0.0221 (10)
Cl70.0368 (10)0.0373 (10)0.0345 (9)0.0143 (6)0.0046 (6)0.0140 (6)
Cl80.0368 (10)0.0373 (10)0.0345 (9)0.0143 (6)0.0046 (6)0.0140 (6)
C290.079 (4)0.079 (4)0.079 (4)0.0324 (16)0.0104 (9)0.0286 (15)
Geometric parameters (Å, º) top
S1—C161.666 (2)C14—C151.391 (3)
O1—C71.220 (3)C14—H140.9500
O2—N51.221 (3)C15—H150.9500
O3—N51.219 (3)C16—N31.399 (2)
N1—C161.353 (2)N3—C171.391 (2)
N1—N21.375 (2)C17—C181.481 (3)
N1—C91.467 (2)C18—H18A0.9800
N2—C171.293 (3)C18—H18B0.9800
N4—C191.283 (3)C18—H18C0.9800
N4—N31.383 (2)C19—C201.469 (3)
N5—C231.475 (3)C19—H190.9500
C1—C21.383 (3)C20—C251.394 (3)
C1—C61.401 (3)C20—C211.401 (3)
C1—H10.9500C21—C221.391 (3)
C2—C31.379 (4)C21—H210.9500
C2—H20.9500C22—C231.371 (3)
C3—C41.394 (4)C22—H220.9500
C3—H30.9500C23—C241.388 (3)
C4—C51.398 (3)C24—C251.379 (3)
C4—H40.9500C24—H240.9500
C5—C61.388 (3)C25—H250.9500
C5—H50.9500Cl1—C261.757 (9)
C6—C71.496 (3)Cl2—C261.696 (9)
C7—C81.510 (3)C26—H26A0.9900
C8—C91.525 (3)C26—H26B0.9900
C8—H8A0.9900C27—Cl41.656 (8)
C8—H8B0.9900C27—Cl31.661 (8)
C9—C101.518 (3)C27—H27A0.9900
C9—H91.0000C27—H27B0.9900
C10—C151.383 (3)C28—Cl51.606 (8)
C10—C111.401 (3)C28—Cl61.671 (8)
C11—C121.388 (3)C28—H28A0.9900
C11—H110.9500C28—H28B0.9900
C12—C131.386 (4)Cl7—C291.718 (11)
C12—H120.9500Cl8—C291.723 (11)
C13—C141.370 (4)C29—H29A0.9900
C13—H130.9500C29—H29B0.9900
C16—N1—N2113.97 (16)N1—C16—S1127.61 (15)
C16—N1—C9125.89 (17)N3—C16—S1130.44 (15)
N2—N1—C9120.04 (16)N4—N3—C17118.17 (16)
C17—N2—N1105.18 (16)N4—N3—C16133.38 (17)
C19—N4—N3119.39 (18)C17—N3—C16108.45 (16)
O3—N5—O2123.6 (2)N2—C17—N3110.44 (18)
O3—N5—C23118.3 (2)N2—C17—C18125.88 (19)
O2—N5—C23118.2 (2)N3—C17—C18123.68 (18)
C2—C1—C6120.0 (2)C17—C18—H18A109.5
C2—C1—H1120.0C17—C18—H18B109.5
C6—C1—H1120.0H18A—C18—H18B109.5
C3—C2—C1120.3 (2)C17—C18—H18C109.5
C3—C2—H2119.9H18A—C18—H18C109.5
C1—C2—H2119.9H18B—C18—H18C109.5
C2—C3—C4120.5 (2)N4—C19—C20118.7 (2)
C2—C3—H3119.8N4—C19—H19120.7
C4—C3—H3119.8C20—C19—H19120.7
C3—C4—C5119.3 (2)C25—C20—C21119.3 (2)
C3—C4—H4120.3C25—C20—C19122.8 (2)
C5—C4—H4120.3C21—C20—C19117.8 (2)
C6—C5—C4120.2 (2)C22—C21—C20120.2 (2)
C6—C5—H5119.9C22—C21—H21119.9
C4—C5—H5119.9C20—C21—H21119.9
C5—C6—C1119.6 (2)C23—C22—C21118.4 (2)
C5—C6—C7122.49 (19)C23—C22—H22120.8
C1—C6—C7117.9 (2)C21—C22—H22120.8
O1—C7—C6120.42 (19)C22—C23—C24123.1 (2)
O1—C7—C8120.74 (19)C22—C23—N5118.9 (2)
C6—C7—C8118.78 (18)C24—C23—N5118.0 (2)
C7—C8—C9111.96 (17)C25—C24—C23118.0 (2)
C7—C8—H8A109.2C25—C24—H24121.0
C9—C8—H8A109.2C23—C24—H24121.0
C7—C8—H8B109.2C24—C25—C20120.9 (2)
C9—C8—H8B109.2C24—C25—H25119.5
H8A—C8—H8B107.9C20—C25—H25119.5
N1—C9—C10108.68 (16)Cl2—C26—Cl1104.9 (6)
N1—C9—C8109.28 (16)Cl2—C26—H26A110.8
C10—C9—C8115.60 (17)Cl1—C26—H26A110.8
N1—C9—H9107.7Cl2—C26—H26B110.8
C10—C9—H9107.7Cl1—C26—H26B110.8
C8—C9—H9107.7H26A—C26—H26B108.8
C15—C10—C11118.4 (2)Cl4—C27—Cl3119.9 (6)
C15—C10—C9123.63 (18)Cl4—C27—H27A107.4
C11—C10—C9118.01 (19)Cl3—C27—H27A107.3
C12—C11—C10120.7 (2)Cl4—C27—H27B107.4
C12—C11—H11119.6Cl3—C27—H27B107.4
C10—C11—H11119.6H27A—C27—H27B106.9
C13—C12—C11119.7 (2)Cl5—C28—Cl6128.9 (7)
C13—C12—H12120.1Cl5—C28—H28A105.1
C11—C12—H12120.1Cl6—C28—H28A105.1
C14—C13—C12120.1 (2)Cl5—C28—H28B105.1
C14—C13—H13120.0Cl6—C28—H28B105.1
C12—C13—H13120.0H28A—C28—H28B105.9
C13—C14—C15120.3 (2)Cl7—C29—Cl8110.7 (10)
C13—C14—H14119.8Cl7—C29—H29A109.5
C15—C14—H14119.8Cl8—C29—H29A109.5
C10—C15—C14120.8 (2)Cl7—C29—H29B109.5
C10—C15—H15119.6Cl8—C29—H29B109.5
C14—C15—H15119.6H29A—C29—H29B108.1
N1—C16—N3101.95 (16)
C16—N1—N2—C171.0 (2)N2—N1—C16—N31.2 (2)
C9—N1—N2—C17177.73 (17)C9—N1—C16—N3177.65 (17)
C6—C1—C2—C31.3 (3)N2—N1—C16—S1179.26 (15)
C1—C2—C3—C41.2 (4)C9—N1—C16—S12.8 (3)
C2—C3—C4—C50.3 (4)C19—N4—N3—C17179.04 (18)
C3—C4—C5—C60.4 (4)C19—N4—N3—C161.0 (3)
C4—C5—C6—C10.3 (3)N1—C16—N3—N4179.15 (19)
C4—C5—C6—C7178.5 (2)S1—C16—N3—N40.4 (3)
C2—C1—C6—C50.5 (3)N1—C16—N3—C170.9 (2)
C2—C1—C6—C7177.69 (19)S1—C16—N3—C17179.57 (16)
C5—C6—C7—O1168.2 (2)N1—N2—C17—N30.4 (2)
C1—C6—C7—O113.7 (3)N1—N2—C17—C18179.9 (2)
C5—C6—C7—C814.6 (3)N4—N3—C17—N2179.70 (17)
C1—C6—C7—C8163.60 (19)C16—N3—C17—N20.3 (2)
O1—C7—C8—C910.1 (3)N4—N3—C17—C180.5 (3)
C6—C7—C8—C9172.62 (18)C16—N3—C17—C18179.4 (2)
C16—N1—C9—C10111.5 (2)N3—N4—C19—C20178.82 (17)
N2—N1—C9—C1064.8 (2)N4—C19—C20—C254.4 (3)
C16—N1—C9—C8121.6 (2)N4—C19—C20—C21177.44 (19)
N2—N1—C9—C862.1 (2)C25—C20—C21—C221.7 (3)
C7—C8—C9—N1161.13 (17)C19—C20—C21—C22179.93 (19)
C7—C8—C9—C1075.9 (2)C20—C21—C22—C230.5 (3)
N1—C9—C10—C15123.7 (2)C21—C22—C23—C240.7 (3)
C8—C9—C10—C150.4 (3)C21—C22—C23—N5179.95 (19)
N1—C9—C10—C1155.4 (2)O3—N5—C23—C22172.5 (2)
C8—C9—C10—C11178.63 (18)O2—N5—C23—C227.6 (3)
C15—C10—C11—C122.3 (3)O3—N5—C23—C248.2 (3)
C9—C10—C11—C12176.8 (2)O2—N5—C23—C24171.8 (2)
C10—C11—C12—C131.0 (4)C22—C23—C24—C250.8 (3)
C11—C12—C13—C140.4 (4)N5—C23—C24—C25179.88 (19)
C12—C13—C14—C150.6 (4)C23—C24—C25—C200.4 (3)
C11—C10—C15—C142.1 (3)C21—C20—C25—C241.6 (3)
C9—C10—C15—C14176.9 (2)C19—C20—C25—C24179.8 (2)
C13—C14—C15—C100.8 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C19—H19···S10.952.433.199 (3)137
C18—H18B···O1i0.982.553.443 (4)152
C22—H22···O1ii0.952.343.202 (3)151
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z.

Experimental details

Crystal data
Chemical formulaC25H21N5O3S·CH2Cl2
Mr556.45
Crystal system, space groupTriclinic, P1
Temperature (K)113
a, b, c (Å)8.9880 (13), 11.4440 (15), 14.8604 (18)
α, β, γ (°)70.212 (11), 88.973 (13), 67.020 (9)
V3)1312.6 (3)
Z2
Radiation typeMo Kα
µ (mm1)0.37
Crystal size (mm)0.26 × 0.24 × 0.20
Data collection
DiffractometerRigaku Saturn CCD
diffractometer
Absorption correctionMulti-scan
(CrystalClear; Rigaku/MSC, 2005)
Tmin, Tmax0.911, 0.931
No. of measured, independent and
observed [I > 2σ(I)] reflections
16932, 6203, 4100
Rint0.035
(sin θ/λ)max1)0.657
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.159, 1.07
No. of reflections6203
No. of parameters396
No. of restraints91
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.27, 0.41

Computer programs: CrystalClear (Rigaku/MSC, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008), CrystalStructure (Rigaku/MSC, 2007).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C19—H19···S10.952.433.199 (3)137
C18—H18B···O1i0.982.553.443 (4)152
C22—H22···O1ii0.952.343.202 (3)151
Symmetry codes: (i) x1, y, z; (ii) x+1, y+1, z.
 

Acknowledgements

The authors gratefully acknowledge support of this project by the Key Laboratory Project of Liaoning Province (grant No. 2008S127) and by the Doctor Starting Foundation of Liaoning Province (grant No. 20071103).

References

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First citationFun, H.-K., Chantrapromma, S., Sujith, K. V. & Kalluraya, B. (2009). Acta Cryst. E65, o495–o496.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationGao, Y., Zhang, L. & Wang, H. (2011). Acta Cryst. E67, o1794.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationRigaku/MSC (2005). CrystalClear. Rigaku/MSC, The Woodlands, Texas, USA.  Google Scholar
First citationRigaku/MSC (2007). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationTan, K. W., Maah, M. J. & Ng, S. W. (2010). Acta Cryst. E66, o2224.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationWang, W., Gao, Y., Xiao, Z., Yao, H. & Zhang, J. (2011). Acta Cryst. E67, o269.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationZhao, B., Liu, Z., Gao, Y., Song, B. & Deng, Q. (2010). Acta Cryst. E66, o2814.  Web of Science CSD CrossRef IUCr Journals Google Scholar

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