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ISSN: 2056-9890

2,6-Bis(2-chloro­ethyl)-8b,8c-di­phenyl­perhydro-2,3a,4a,6,7a,8a-hexa­aza­cyclo­penta­[def]fluorene-4,8-di­thione

aKey Laboratory of Pesticides and Chemical Biology of the Ministry of Education, College of Chemistry, Central China Normal University, Wuhan 430079, People's Republic of China
*Correspondence e-mail: wyd851201@126.com

(Received 16 June 2009; accepted 23 June 2009; online 27 June 2009)

In the title mol­ecule, C24H26Cl2N6S2, the two phenyl rings form a dihedral angle of 51.95 (7)° and the distance between their centroids is 4.156 (8) Å. The crystal packing exhibits weak inter­molecular C—H⋯S and C—H⋯N hydrogen bonds.

Related literature

For applications of glycoluril derivatives, see: Wu et al. (2002[Wu, A., Chakraborty, A., Witl, D., Lagona, J., Damkaci, F., Ofori, M. A., Chiles, J. K., Fettinger, J. C. & Isaacs, L. (2002). J. Org. Chem. 67, 5817-5830.]). For a related structure, see: Wang & Xi (2009[Wang, Z. & Xi, H. (2009). Acta Cryst. E65, o1426.]). For details of the synthesis, see: Ramos & Rosen (1981[Ramos, S. & Rosen, W. (1981). J. Org. Chem. 46, 3530-3533.]).

[Scheme 1]

Experimental

Crystal data
  • C24H26Cl2N6S2

  • Mr = 533.53

  • Monoclinic, P 21 /c

  • a = 8.7566 (2) Å

  • b = 14.0877 (3) Å

  • c = 20.8575 (5) Å

  • β = 99.525 (1)°

  • V = 2537.52 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.45 mm−1

  • T = 298 K

  • 0.23 × 0.20 × 0.10 mm

Data collection
  • Bruker SMART 4K CCD area-detector diffractometer

  • Absorption correction: none

  • 16129 measured reflections

  • 4979 independent reflections

  • 3375 reflections with I > 2σ(I)

  • Rint = 0.078

Refinement
  • R[F2 > 2σ(F2)] = 0.064

  • wR(F2) = 0.164

  • S = 1.02

  • 4979 reflections

  • 307 parameters

  • H-atom parameters constrained

  • Δρmax = 0.63 e Å−3

  • Δρmin = −0.51 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C24—H24B⋯N1i 0.97 2.55 3.485 (4) 162
C22—H22B⋯S1ii 0.97 2.80 3.607 (3) 141
Symmetry codes: (i) x-1, y, z; (ii) [-x, y+{\script{1\over 2}}, -z+{\script{1\over 2}}].

Data collection: SMART (Bruker, 1997[Bruker (1997). SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 1999[Bruker (1999). SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; 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: SHELXL97.

Supporting information


Comment top

Glycoluril derivatives have many areas of applications, such as explosives, slow-release fertilizers, cross-linkers, stabilizers of organic compounds against photodegradation, and as reagents in combinatorial chemistry (Wu et al., 2002). Also, The rigid concave shape of glycoluril makes it a versatile building block to construct various supramolecular objects (Wang & Xi, 2009). We report here the structure of the title thioglycoluril derivative (Fig. 1), which is a potential receptor in supramolecular chemistry.

In the title compound all bond lengths and angles are normal and comparable with those observed in the related structure (Wang & Xi, 2009). The crystal packing is stabilized by intermolecular C–H···S and C—H···N hydrogen bonds (Table 1).

Related literature top

For applications of glycoluril derivatives, see: Wu et al. (2002). For a related structure, see: Wang & Xi (2009). For details of the synthesis, see: Ramos & Rosen (1981).

Experimental top

The title compound was synthesized according to the procedure reported by Ramos & Rosen (1981). Crystals appropriate for X-ray data collection were obtained by slow evaporation of the dichloromethane solution at 293 K.

Refinement top

All H atoms were initially located in a difference Fourier map and then included with constrained bond lengths and isotropic displacement parameters: C—H = 0.93 Å and Uĩso~(H) = 1.2 U~eq~(C) for aromatic H atoms, C—H = 0.97 Å and Uĩso~(H) = 1.2 U~eq~(C) for methylene H atoms, C—H = 0.96 Å and Uĩso~(H) = 1.5 U~eq~(C) for methyl H atoms.

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT (Bruker, 1999); 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 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. View of (I) showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented by spheres of arbitrary radius.
2,6-Bis(2-chloroethyl)-8b,8c-diphenylperhydro-2,3a,4a,6,7a,8a- hexaazacyclopenta[def]fluorene-4,8-dithione top
Crystal data top
C24H26Cl2N6S2F(000) = 1112
Mr = 533.53Dx = 1.397 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2851 reflections
a = 8.7566 (2) Åθ = 2.5–21.7°
b = 14.0877 (3) ŵ = 0.45 mm1
c = 20.8575 (5) ÅT = 298 K
β = 99.525 (1)°Block, colourless
V = 2537.52 (10) Å30.23 × 0.20 × 0.10 mm
Z = 4
Data collection top
Bruker SMART 4K CCD area-detector
diffractometer
3375 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.078
Graphite monochromatorθmax = 26.0°, θmin = 1.8°
ϕ and ω scansh = 1010
16129 measured reflectionsk = 1717
4979 independent reflectionsl = 1825
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)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.164H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0798P)2]
where P = (Fo2 + 2Fc2)/3
4979 reflections(Δ/σ)max < 0.001
307 parametersΔρmax = 0.63 e Å3
0 restraintsΔρmin = 0.51 e Å3
Crystal data top
C24H26Cl2N6S2V = 2537.52 (10) Å3
Mr = 533.53Z = 4
Monoclinic, P21/cMo Kα radiation
a = 8.7566 (2) ŵ = 0.45 mm1
b = 14.0877 (3) ÅT = 298 K
c = 20.8575 (5) Å0.23 × 0.20 × 0.10 mm
β = 99.525 (1)°
Data collection top
Bruker SMART 4K CCD area-detector
diffractometer
3375 reflections with I > 2σ(I)
16129 measured reflectionsRint = 0.078
4979 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0640 restraints
wR(F2) = 0.164H-atom parameters constrained
S = 1.02Δρmax = 0.63 e Å3
4979 reflectionsΔρmin = 0.51 e Å3
307 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*/Ueq
C10.5265 (5)0.0996 (4)0.4154 (2)0.0757 (13)
H1A0.44970.08980.44340.091*
H1B0.54580.16730.41360.091*
C20.4639 (4)0.0657 (3)0.34973 (18)0.0501 (9)
H2A0.44660.00220.35160.060*
H2B0.36420.09560.33560.060*
C30.5429 (3)0.0178 (2)0.24750 (17)0.0394 (8)
H3A0.53660.04610.26410.047*
H3B0.63240.02100.22570.047*
C40.5586 (4)0.1811 (2)0.27789 (16)0.0393 (8)
H4A0.64830.19250.25720.047*
H4B0.56430.22420.31450.047*
C50.2613 (3)0.0038 (2)0.19965 (15)0.0319 (7)
C60.2848 (3)0.2397 (2)0.24636 (15)0.0314 (7)
C70.3878 (3)0.13561 (19)0.17632 (14)0.0281 (7)
C80.4933 (3)0.1550 (2)0.12701 (15)0.0342 (7)
C90.5363 (4)0.0818 (3)0.08934 (17)0.0493 (9)
H90.50210.02030.09470.059*
C100.6305 (5)0.1006 (4)0.0436 (2)0.0679 (13)
H100.65920.05160.01820.081*
C110.6819 (5)0.1918 (4)0.0354 (2)0.0725 (14)
H110.74450.20410.00440.087*
C120.6409 (4)0.2640 (3)0.0727 (2)0.0670 (12)
H120.67630.32530.06760.080*
C130.5465 (4)0.2455 (3)0.11833 (18)0.0494 (9)
H130.51840.29490.14360.059*
C140.2095 (3)0.14683 (19)0.15257 (14)0.0278 (7)
C150.1585 (3)0.1754 (2)0.08262 (15)0.0336 (7)
C160.1323 (4)0.1075 (3)0.03430 (17)0.0496 (9)
H160.14400.04360.04500.060*
C170.0888 (5)0.1341 (3)0.02984 (19)0.0687 (12)
H170.07190.08790.06210.082*
C180.0703 (5)0.2282 (4)0.0463 (2)0.0752 (14)
H180.03920.24580.08940.090*
C190.0978 (5)0.2958 (3)0.0012 (2)0.0714 (13)
H190.08700.35970.00980.086*
C200.1416 (4)0.2694 (3)0.06534 (18)0.0522 (10)
H200.15990.31590.09730.063*
C210.0141 (3)0.0516 (2)0.17475 (16)0.0345 (7)
H21A0.07840.06570.13340.041*
H21B0.04040.01170.18760.041*
C220.0005 (3)0.2145 (2)0.20563 (17)0.0384 (8)
H22A0.06280.23410.16520.046*
H22B0.01630.25930.23910.046*
C230.0225 (4)0.0944 (2)0.28981 (15)0.0383 (8)
H23A0.01570.14850.31800.046*
H23B0.13130.08060.29060.046*
C240.0531 (4)0.0101 (2)0.31604 (17)0.0429 (8)
H24A0.05890.04250.28570.052*
H24B0.15730.02620.32230.052*
Cl10.69817 (17)0.04249 (16)0.44949 (7)0.1337 (8)
Cl20.06244 (11)0.02216 (7)0.39222 (5)0.0585 (3)
N10.5631 (3)0.08436 (18)0.30145 (13)0.0382 (7)
N20.4172 (3)0.20160 (16)0.23108 (12)0.0304 (6)
N30.4014 (3)0.03855 (16)0.20014 (13)0.0301 (6)
N40.1644 (3)0.21709 (16)0.19809 (12)0.0303 (6)
N50.1496 (3)0.05305 (16)0.16642 (12)0.0289 (6)
N60.0485 (3)0.11945 (18)0.22321 (13)0.0356 (6)
S10.23332 (10)0.10921 (6)0.23090 (5)0.0516 (3)
S20.27222 (11)0.30702 (6)0.31074 (4)0.0461 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.065 (3)0.104 (4)0.059 (3)0.015 (3)0.015 (2)0.001 (3)
C20.041 (2)0.064 (2)0.045 (2)0.0041 (17)0.0059 (17)0.0122 (19)
C30.0314 (17)0.0371 (18)0.049 (2)0.0063 (14)0.0052 (16)0.0086 (16)
C40.0339 (18)0.0444 (19)0.040 (2)0.0068 (14)0.0066 (15)0.0017 (16)
C50.0287 (16)0.0280 (16)0.040 (2)0.0012 (12)0.0087 (14)0.0048 (14)
C60.0374 (17)0.0230 (15)0.0350 (19)0.0003 (12)0.0097 (15)0.0045 (13)
C70.0300 (16)0.0241 (15)0.0307 (17)0.0008 (12)0.0068 (13)0.0010 (13)
C80.0279 (16)0.0418 (19)0.0333 (18)0.0004 (13)0.0061 (14)0.0005 (15)
C90.042 (2)0.061 (2)0.047 (2)0.0026 (17)0.0154 (18)0.0076 (19)
C100.050 (2)0.112 (4)0.046 (3)0.015 (2)0.023 (2)0.014 (2)
C110.047 (2)0.124 (4)0.051 (3)0.011 (3)0.021 (2)0.016 (3)
C120.057 (3)0.088 (3)0.058 (3)0.022 (2)0.015 (2)0.019 (3)
C130.057 (2)0.051 (2)0.043 (2)0.0113 (17)0.0161 (18)0.0069 (17)
C140.0305 (16)0.0233 (15)0.0313 (17)0.0030 (12)0.0105 (13)0.0017 (13)
C150.0329 (17)0.0358 (17)0.0340 (19)0.0058 (13)0.0113 (14)0.0005 (14)
C160.070 (3)0.044 (2)0.036 (2)0.0072 (18)0.0130 (19)0.0031 (17)
C170.102 (4)0.073 (3)0.031 (2)0.007 (3)0.011 (2)0.009 (2)
C180.093 (4)0.102 (4)0.032 (2)0.020 (3)0.016 (2)0.022 (3)
C190.103 (4)0.063 (3)0.051 (3)0.023 (2)0.019 (3)0.024 (2)
C200.073 (3)0.042 (2)0.043 (2)0.0065 (18)0.012 (2)0.0064 (18)
C210.0276 (16)0.0409 (18)0.0349 (19)0.0010 (13)0.0048 (14)0.0002 (15)
C220.0340 (17)0.0412 (19)0.041 (2)0.0118 (14)0.0105 (15)0.0007 (16)
C230.0374 (18)0.0450 (19)0.034 (2)0.0018 (15)0.0086 (15)0.0027 (15)
C240.0354 (18)0.053 (2)0.041 (2)0.0052 (15)0.0065 (16)0.0053 (17)
Cl10.0874 (10)0.253 (2)0.0537 (8)0.0758 (12)0.0083 (7)0.0002 (10)
Cl20.0556 (6)0.0663 (6)0.0516 (6)0.0015 (5)0.0029 (5)0.0170 (5)
N10.0297 (14)0.0429 (16)0.0413 (17)0.0002 (12)0.0033 (12)0.0062 (13)
N20.0316 (14)0.0296 (13)0.0307 (15)0.0033 (11)0.0076 (11)0.0015 (11)
N30.0241 (13)0.0236 (13)0.0426 (16)0.0012 (10)0.0058 (11)0.0019 (11)
N40.0342 (14)0.0255 (13)0.0319 (15)0.0052 (10)0.0077 (12)0.0022 (11)
N50.0270 (13)0.0264 (13)0.0340 (15)0.0008 (10)0.0074 (11)0.0005 (11)
N60.0320 (14)0.0409 (16)0.0356 (16)0.0058 (11)0.0105 (12)0.0000 (12)
S10.0454 (5)0.0260 (5)0.0856 (8)0.0009 (4)0.0169 (5)0.0123 (5)
S20.0600 (6)0.0389 (5)0.0420 (6)0.0011 (4)0.0163 (5)0.0135 (4)
Geometric parameters (Å, º) top
C1—C21.469 (6)C12—C131.384 (5)
C1—Cl11.749 (4)C12—H120.9300
C1—H1A0.9700C13—H130.9300
C1—H1B0.9700C14—N51.468 (3)
C2—N11.459 (4)C14—N41.470 (3)
C2—H2A0.9700C14—C151.508 (4)
C2—H2B0.9700C15—C201.374 (4)
C3—N11.453 (4)C15—C161.381 (4)
C3—N31.480 (4)C16—C171.381 (5)
C3—H3A0.9700C16—H160.9300
C3—H3B0.9700C17—C181.372 (6)
C4—N11.447 (4)C17—H170.9300
C4—N21.473 (4)C18—C191.366 (6)
C4—H4A0.9700C18—H180.9300
C4—H4B0.9700C19—C201.381 (5)
C5—N51.362 (4)C19—H190.9300
C5—N31.363 (4)C20—H200.9300
C5—S11.656 (3)C21—N61.458 (4)
C6—N21.362 (4)C21—N51.472 (4)
C6—N41.369 (4)C21—H21A0.9700
C6—S21.662 (3)C21—H21B0.9700
C7—N31.453 (3)C22—N41.470 (4)
C7—N21.462 (4)C22—N61.471 (4)
C7—C81.517 (4)C22—H22A0.9700
C7—C141.565 (4)C22—H22B0.9700
C8—C131.379 (4)C23—N61.468 (4)
C8—C91.385 (4)C23—C241.506 (4)
C9—C101.386 (5)C23—H23A0.9700
C9—H90.9300C23—H23B0.9700
C10—C111.381 (6)C24—Cl21.795 (3)
C10—H100.9300C24—H24A0.9700
C11—C121.364 (6)C24—H24B0.9700
C11—H110.9300
C2—C1—Cl1113.1 (3)C20—C15—C16118.6 (3)
C2—C1—H1A109.0C20—C15—C14120.8 (3)
Cl1—C1—H1A109.0C16—C15—C14120.5 (3)
C2—C1—H1B109.0C17—C16—C15120.4 (3)
Cl1—C1—H1B109.0C17—C16—H16119.8
H1A—C1—H1B107.8C15—C16—H16119.8
N1—C2—C1114.3 (3)C18—C17—C16120.4 (4)
N1—C2—H2A108.7C18—C17—H17119.8
C1—C2—H2A108.7C16—C17—H17119.8
N1—C2—H2B108.7C19—C18—C17119.6 (4)
C1—C2—H2B108.7C19—C18—H18120.2
H2A—C2—H2B107.6C17—C18—H18120.2
N1—C3—N3111.8 (2)C18—C19—C20120.1 (4)
N1—C3—H3A109.3C18—C19—H19120.0
N3—C3—H3A109.3C20—C19—H19120.0
N1—C3—H3B109.3C15—C20—C19121.0 (4)
N3—C3—H3B109.3C15—C20—H20119.5
H3A—C3—H3B107.9C19—C20—H20119.5
N1—C4—N2112.5 (2)N6—C21—N5112.9 (2)
N1—C4—H4A109.1N6—C21—H21A109.0
N2—C4—H4A109.1N5—C21—H21A109.0
N1—C4—H4B109.1N6—C21—H21B109.0
N2—C4—H4B109.1N5—C21—H21B109.0
H4A—C4—H4B107.8H21A—C21—H21B107.8
N5—C5—N3108.4 (2)N4—C22—N6112.3 (2)
N5—C5—S1126.0 (2)N4—C22—H22A109.1
N3—C5—S1125.5 (2)N6—C22—H22A109.1
N2—C6—N4108.5 (3)N4—C22—H22B109.1
N2—C6—S2125.9 (2)N6—C22—H22B109.1
N4—C6—S2125.5 (2)H22A—C22—H22B107.9
N3—C7—N2109.7 (2)N6—C23—C24113.0 (3)
N3—C7—C8112.1 (2)N6—C23—H23A109.0
N2—C7—C8111.5 (2)C24—C23—H23A109.0
N3—C7—C14103.0 (2)N6—C23—H23B109.0
N2—C7—C14102.7 (2)C24—C23—H23B109.0
C8—C7—C14117.1 (2)H23A—C23—H23B107.8
C13—C8—C9118.9 (3)C23—C24—Cl2107.7 (2)
C13—C8—C7120.8 (3)C23—C24—H24A110.2
C9—C8—C7120.3 (3)Cl2—C24—H24A110.2
C10—C9—C8119.8 (4)C23—C24—H24B110.2
C10—C9—H9120.1Cl2—C24—H24B110.2
C8—C9—H9120.1H24A—C24—H24B108.5
C11—C10—C9120.4 (4)C4—N1—C3110.6 (3)
C11—C10—H10119.8C4—N1—C2114.7 (3)
C9—C10—H10119.8C3—N1—C2114.1 (3)
C12—C11—C10120.0 (4)C6—N2—C7112.7 (2)
C12—C11—H11120.0C6—N2—C4125.2 (3)
C10—C11—H11120.0C7—N2—C4114.4 (2)
C11—C12—C13119.7 (4)C5—N3—C7112.7 (2)
C11—C12—H12120.1C5—N3—C3124.9 (3)
C13—C12—H12120.1C7—N3—C3115.2 (2)
C8—C13—C12121.2 (4)C6—N4—C14112.0 (2)
C8—C13—H13119.4C6—N4—C22125.0 (3)
C12—C13—H13119.4C14—N4—C22115.1 (2)
N5—C14—N4109.6 (2)C5—N5—C14112.3 (2)
N5—C14—C15111.8 (2)C5—N5—C21124.3 (2)
N4—C14—C15112.1 (2)C14—N5—C21115.0 (2)
N5—C14—C7102.5 (2)C21—N6—C23113.2 (2)
N4—C14—C7102.9 (2)C21—N6—C22108.8 (2)
C15—C14—C7117.0 (2)C23—N6—C22111.1 (3)
Cl1—C1—C2—N163.9 (4)C8—C7—N2—C6132.9 (3)
N3—C7—C8—C13153.4 (3)C14—C7—N2—C66.7 (3)
N2—C7—C8—C1329.9 (4)N3—C7—N2—C448.9 (3)
C14—C7—C8—C1388.0 (4)C8—C7—N2—C475.9 (3)
N3—C7—C8—C927.4 (4)C14—C7—N2—C4157.9 (2)
N2—C7—C8—C9150.9 (3)N1—C4—N2—C693.6 (3)
C14—C7—C8—C991.2 (3)N1—C4—N2—C753.5 (3)
C13—C8—C9—C100.4 (5)N5—C5—N3—C710.2 (3)
C7—C8—C9—C10178.8 (3)S1—C5—N3—C7172.8 (2)
C8—C9—C10—C110.1 (6)N5—C5—N3—C3158.9 (3)
C9—C10—C11—C120.4 (7)S1—C5—N3—C324.0 (4)
C10—C11—C12—C130.6 (7)N2—C7—N3—C5103.0 (3)
C9—C8—C13—C120.2 (5)C8—C7—N3—C5132.5 (3)
C7—C8—C13—C12179.0 (3)C14—C7—N3—C55.8 (3)
C11—C12—C13—C80.3 (6)N2—C7—N3—C348.9 (3)
N3—C7—C14—N50.4 (3)C8—C7—N3—C375.5 (3)
N2—C7—C14—N5114.4 (2)C14—C7—N3—C3157.8 (2)
C8—C7—C14—N5123.1 (3)N1—C3—N3—C595.3 (3)
N3—C7—C14—N4113.5 (2)N1—C3—N3—C752.8 (3)
N2—C7—C14—N40.6 (3)N2—C6—N4—C1410.1 (3)
C8—C7—C14—N4123.1 (3)S2—C6—N4—C14172.8 (2)
N3—C7—C14—C15123.1 (3)N2—C6—N4—C22157.3 (2)
N2—C7—C14—C15122.9 (3)S2—C6—N4—C2225.5 (4)
C8—C7—C14—C150.3 (4)N5—C14—N4—C6102.9 (3)
N5—C14—C15—C20151.7 (3)C15—C14—N4—C6132.2 (3)
N4—C14—C15—C2028.1 (4)C7—C14—N4—C65.6 (3)
C7—C14—C15—C2090.5 (3)N5—C14—N4—C2247.8 (3)
N5—C14—C15—C1630.2 (4)C15—C14—N4—C2277.1 (3)
N4—C14—C15—C16153.9 (3)C7—C14—N4—C22156.4 (2)
C7—C14—C15—C1687.5 (4)N6—C22—N4—C692.4 (3)
C20—C15—C16—C170.5 (5)N6—C22—N4—C1454.0 (3)
C14—C15—C16—C17178.6 (3)N3—C5—N5—C1410.4 (3)
C15—C16—C17—C180.3 (6)S1—C5—N5—C14172.6 (2)
C16—C17—C18—C191.1 (7)N3—C5—N5—C21156.7 (3)
C17—C18—C19—C201.0 (7)S1—C5—N5—C2126.3 (4)
C16—C15—C20—C190.7 (5)N4—C14—N5—C5102.4 (3)
C14—C15—C20—C19178.7 (3)C15—C14—N5—C5132.6 (3)
C18—C19—C20—C150.1 (7)C7—C14—N5—C56.5 (3)
N6—C23—C24—Cl2171.8 (2)N4—C14—N5—C2147.2 (3)
N2—C4—N1—C354.4 (3)C15—C14—N5—C2177.8 (3)
N2—C4—N1—C276.3 (3)C7—C14—N5—C21156.1 (2)
N3—C3—N1—C453.6 (3)N6—C21—N5—C592.0 (3)
N3—C3—N1—C277.5 (3)N6—C21—N5—C1453.5 (3)
C1—C2—N1—C477.7 (4)N5—C21—N6—C2368.8 (3)
C1—C2—N1—C3153.3 (3)N5—C21—N6—C2255.2 (3)
N4—C6—N2—C710.6 (3)C24—C23—N6—C2171.7 (3)
S2—C6—N2—C7172.3 (2)C24—C23—N6—C22165.6 (2)
N4—C6—N2—C4158.2 (3)N4—C22—N6—C2155.4 (3)
S2—C6—N2—C424.7 (4)N4—C22—N6—C2369.9 (3)
N3—C7—N2—C6102.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C24—H24B···N1i0.972.553.485 (4)162
C22—H22B···S1ii0.972.803.607 (3)141
Symmetry codes: (i) x1, y, z; (ii) x, y+1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC24H26Cl2N6S2
Mr533.53
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)8.7566 (2), 14.0877 (3), 20.8575 (5)
β (°) 99.525 (1)
V3)2537.52 (10)
Z4
Radiation typeMo Kα
µ (mm1)0.45
Crystal size (mm)0.23 × 0.20 × 0.10
Data collection
DiffractometerBruker SMART 4K CCD area-detector
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
16129, 4979, 3375
Rint0.078
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.064, 0.164, 1.02
No. of reflections4979
No. of parameters307
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.63, 0.51

Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1999), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C24—H24B···N1i0.972.553.485 (4)161.8
C22—H22B···S1ii0.972.803.607 (3)141.4
Symmetry codes: (i) x1, y, z; (ii) x, y+1/2, z+1/2.
 

Acknowledgements

The authors thank Professor An-Xin Wu for technical assistance and Dr Meng Xiang-Gao for the data collection.

References

First citationBruker (1997). SMART. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationBruker (1999). SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationRamos, S. & Rosen, W. (1981). J. Org. Chem. 46, 3530–3533.  CrossRef CAS Web of Science Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationWang, Z. & Xi, H. (2009). Acta Cryst. E65, o1426.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationWu, A., Chakraborty, A., Witl, D., Lagona, J., Damkaci, F., Ofori, M. A., Chiles, J. K., Fettinger, J. C. & Isaacs, L. (2002). J. Org. Chem. 67, 5817–5830.  Web of Science CSD CrossRef PubMed CAS Google Scholar

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