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

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COMMUNICATIONS
ISSN: 2056-9890

N,N′-Bis(3,3-di­methyl­all­yl)-N,N′-(prop­ane-1,3-diyl)di­benzene­sulfonamide

aMaterials Chemistry Laboratory, Department of Chemistry, GC University, Lahore 54000, Pakistan, and bDepartment of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland
*Correspondence e-mail: iuklodhi@yahoo.com

(Received 1 November 2011; accepted 24 November 2011; online 30 November 2011)

In the title compound, C25H34N2O4S2, the conformation of the linking N—C—C—C—N chain is gauche-anti [torsion angles = −68.49 (19) and 167.95 (14)°]. The dihedral angle between the aromatic rings is 89.64 (6)°.

Related literature

For the related structures of N-[3-(benzene­sulfonamido)­prop­yl]benzene­sulfonamide and N,N′-(propane-1,3-di­yl)bis­(p-toluene­sulfonamide), see: Sheikh et al. (2011[Sheikh, T. A., Khan, I. U., Harrison, W. T. A. & Ejaz, (2011). Acta Cryst. E67, o1737.]) and Khan et al. (2011[Khan, I. U., Sheikh, T. A., Ejaz, & Harrison, W. T. A. (2011). Acta Cryst. E67, o2371.]), respectively.

[Scheme 1]

Experimental

Crystal data
  • C25H34N2O4S2

  • Mr = 490.66

  • Monoclinic, P 21 /n

  • a = 10.3019 (2) Å

  • b = 16.3962 (4) Å

  • c = 16.0500 (4) Å

  • β = 108.449 (1)°

  • V = 2571.71 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.24 mm−1

  • T = 296 K

  • 0.50 × 0.25 × 0.20 mm

Data collection
  • Bruker APEXII CCD diffractometer

  • 40701 measured reflections

  • 5059 independent reflections

  • 4011 reflections with I > 2σ(I)

  • Rint = 0.028

Refinement
  • R[F2 > 2σ(F2)] = 0.034

  • wR(F2) = 0.102

  • S = 1.05

  • 5059 reflections

  • 302 parameters

  • H-atom parameters constrained

  • Δρmax = 0.25 e Å−3

  • Δρmin = −0.24 e Å−3

Data collection: APEX2 (Bruker, 2007[Bruker (2007). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2007[Bruker (2007). APEX2 and 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: ORTEP-3 (Farrugia, 1997[Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.]); software used to prepare material for publication: SHELXL97.

Supporting information


Comment top

As part of our ongoing structural studies of symmetric sulfonamides with a linking propyl chain, including N-[3-(benzenesulfonamido)propyl]benzenesulfonamide (II) (Sheikh et al., 2011) and N,N'-(propane-1,3-diyl)bis(p-toluenesulfonamide) (III) (Khan et al., 2011), the synthesis and structure of the title compound, C25H34N2O4S2 (I), (Fig. 1), are now described.

The dihedral angle between the phenyl rings in the title compound (I) is 89.64 (6)°. The conformations of the atoms of the central chain are gauche-anti [torsion angles N1—C7—C8—C8 = -68.49 (19)° and C7—C8—C9—N2 = 167.95 (14)°]. The S1—N1—C7—C8 and S2—N2—C9—C8 torsion angles are 116.52 (14)° and -98.69 (16)°, respectively. The bond-angle sums for N1 and N2 are 349.5 and 356.0°, respectively, indicating a significantly greater departure from planarity for N1. In the crystal of (I), only van der Waals' forces are present.

In compound (II) (Sheikh et al., 2011), the conformation of the central N—C—C—C—N chain is gauche-gauche [torsion angles = 72.5 (5) and 65.7 (5)°]. In compound (III) (Khan et al., 2011), the complete molecule is generated by crystallographic twofold symmetry and the two N—C—C—C fragments have the same gauche conformation [torsion angle = 75.53 (14)°].

Related literature top

For the related structures of N-[3-(benzenesulfonamido)propyl]benzenesulfonamide and N,N'-(propane-1,3-diyl)bis(p-toluenesulfonamide), see: Sheikh et al. (2011) and Khan et al. (2011), respectively.

Experimental top

A mixture of N-[3-(benzenesulfonamido)propyl]benzenesulfonamide (0.177 g, 0.5 mmol), sodium hydride (0.24 g; 1.0 mmol) and N,N-dimethylformamide (10.0 ml) was stirred in a 100 ml round-bottom flask at room temperature for 30 minutes followed by the addition of 3,3-dimethylallyl bromide (0.116 ml; 1.0 mmol). The reaction mixture was stirred for six hours with reaction progress monitored by TLC. At the end of the reaction, the contents were poured over crushed ice. The precipitated product was isolated, washed and recrystallized from methanol to yield colorless blocks.

Refinement top

The hydrogen atoms were placed in calculated positions (C—H = 0.97–0.98 Å) and refined as riding atoms with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C). The methyl groups were allowed to rotate, but not to tip, to best fit the electron density.

Structure description top

As part of our ongoing structural studies of symmetric sulfonamides with a linking propyl chain, including N-[3-(benzenesulfonamido)propyl]benzenesulfonamide (II) (Sheikh et al., 2011) and N,N'-(propane-1,3-diyl)bis(p-toluenesulfonamide) (III) (Khan et al., 2011), the synthesis and structure of the title compound, C25H34N2O4S2 (I), (Fig. 1), are now described.

The dihedral angle between the phenyl rings in the title compound (I) is 89.64 (6)°. The conformations of the atoms of the central chain are gauche-anti [torsion angles N1—C7—C8—C8 = -68.49 (19)° and C7—C8—C9—N2 = 167.95 (14)°]. The S1—N1—C7—C8 and S2—N2—C9—C8 torsion angles are 116.52 (14)° and -98.69 (16)°, respectively. The bond-angle sums for N1 and N2 are 349.5 and 356.0°, respectively, indicating a significantly greater departure from planarity for N1. In the crystal of (I), only van der Waals' forces are present.

In compound (II) (Sheikh et al., 2011), the conformation of the central N—C—C—C—N chain is gauche-gauche [torsion angles = 72.5 (5) and 65.7 (5)°]. In compound (III) (Khan et al., 2011), the complete molecule is generated by crystallographic twofold symmetry and the two N—C—C—C fragments have the same gauche conformation [torsion angle = 75.53 (14)°].

For the related structures of N-[3-(benzenesulfonamido)propyl]benzenesulfonamide and N,N'-(propane-1,3-diyl)bis(p-toluenesulfonamide), see: Sheikh et al. (2011) and Khan et al. (2011), respectively.

Computing details top

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular conformation and atom mumbering scheme for (I) showing 50% probability displacement ellipsoids.
N,N'-Bis(3,3-dimethylallyl)-N,N'- (propane-1,3-diyl)dibenzenesulfonamide top
Crystal data top
C25H34N2O4S2F(000) = 1048
Mr = 490.66Dx = 1.267 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 4846 reflections
a = 10.3019 (2) Åθ = 2.4–28.3°
b = 16.3962 (4) ŵ = 0.24 mm1
c = 16.0500 (4) ÅT = 296 K
β = 108.449 (1)°Faceted block, colourless
V = 2571.71 (10) Å30.50 × 0.25 × 0.20 mm
Z = 4
Data collection top
Bruker APEXII CCD
diffractometer
4011 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.028
Graphite monochromatorθmax = 26.0°, θmin = 2.4°
ω scansh = 1212
40701 measured reflectionsk = 2020
5059 independent reflectionsl = 1919
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)] = 0.034Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.102H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0458P)2 + 0.7949P]
where P = (Fo2 + 2Fc2)/3
5059 reflections(Δ/σ)max = 0.001
302 parametersΔρmax = 0.25 e Å3
0 restraintsΔρmin = 0.24 e Å3
Crystal data top
C25H34N2O4S2V = 2571.71 (10) Å3
Mr = 490.66Z = 4
Monoclinic, P21/nMo Kα radiation
a = 10.3019 (2) ŵ = 0.24 mm1
b = 16.3962 (4) ÅT = 296 K
c = 16.0500 (4) Å0.50 × 0.25 × 0.20 mm
β = 108.449 (1)°
Data collection top
Bruker APEXII CCD
diffractometer
4011 reflections with I > 2σ(I)
40701 measured reflectionsRint = 0.028
5059 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0340 restraints
wR(F2) = 0.102H-atom parameters constrained
S = 1.05Δρmax = 0.25 e Å3
5059 reflectionsΔρmin = 0.24 e Å3
302 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
C10.21354 (16)0.05844 (10)0.30778 (10)0.0423 (4)
C20.1634 (2)0.13588 (11)0.31257 (12)0.0552 (4)
H20.08780.14340.33150.066*
C30.2272 (3)0.20195 (12)0.28881 (13)0.0702 (6)
H30.19480.25430.29240.084*
C40.3379 (2)0.19098 (15)0.26002 (14)0.0741 (6)
H40.38030.23580.24430.089*
C50.3857 (2)0.11425 (15)0.25434 (14)0.0693 (6)
H50.46030.10700.23420.083*
C60.32444 (18)0.04722 (12)0.27827 (12)0.0533 (4)
H60.35750.00500.27450.064*
C70.34337 (16)0.07689 (10)0.48435 (11)0.0475 (4)
H7A0.37580.09290.43620.057*
H7B0.41040.04020.52200.057*
C80.33084 (19)0.15195 (11)0.53634 (11)0.0520 (4)
H8A0.28910.13670.58040.062*
H8B0.42160.17290.56660.062*
C90.24648 (18)0.21859 (10)0.47923 (11)0.0455 (4)
H9A0.29770.24180.44370.055*
H9B0.16340.19490.43980.055*
C100.06124 (17)0.30932 (12)0.43729 (11)0.0525 (4)
C110.10347 (19)0.25338 (14)0.36942 (12)0.0602 (5)
H110.07250.19980.37730.072*
C120.1930 (2)0.27902 (17)0.28927 (13)0.0721 (6)
H120.22020.24250.24260.087*
C130.2414 (2)0.35669 (18)0.27828 (16)0.0784 (7)
H130.30240.37270.22450.094*
C140.2010 (2)0.41129 (17)0.34560 (17)0.0815 (7)
H140.23520.46420.33770.098*
C150.1093 (2)0.38832 (14)0.42576 (14)0.0684 (5)
H150.08050.42590.47130.082*
C160.17868 (17)0.02590 (10)0.50808 (11)0.0466 (4)
H16A0.09130.05100.47750.056*
H16B0.16910.00260.55880.056*
C170.28411 (17)0.09122 (10)0.53891 (12)0.0500 (4)
H170.30220.12280.49570.060*
C180.35404 (17)0.10877 (11)0.62076 (12)0.0507 (4)
C190.4535 (2)0.17811 (14)0.64300 (18)0.0794 (7)
H19A0.42790.21570.68090.119*
H19B0.54370.15750.67230.119*
H19C0.45290.20560.59010.119*
C200.3395 (2)0.06355 (14)0.69819 (13)0.0698 (6)
H20A0.42420.06590.74560.105*
H20B0.26820.08800.71640.105*
H20C0.31670.00770.68230.105*
C210.26420 (19)0.36620 (11)0.52107 (14)0.0598 (5)
H21A0.22300.40640.54920.072*
H21B0.24010.38000.45930.072*
C220.41617 (19)0.36853 (11)0.56158 (13)0.0570 (5)
H220.44990.35900.62170.068*
C230.50789 (19)0.38257 (10)0.52170 (12)0.0534 (4)
C240.6577 (2)0.38660 (15)0.57265 (16)0.0778 (6)
H24A0.70530.34410.55310.117*
H24B0.67010.37960.63410.117*
H24C0.69350.43870.56340.117*
C250.4767 (2)0.39749 (13)0.42503 (13)0.0687 (5)
H25A0.52870.36040.40190.103*
H25B0.50060.45250.41570.103*
H25C0.38080.38910.39570.103*
S10.13963 (4)0.02601 (3)0.34402 (3)0.04583 (13)
S20.05674 (5)0.27959 (3)0.53939 (3)0.05475 (14)
N10.21229 (13)0.03391 (8)0.44902 (8)0.0415 (3)
N20.20938 (14)0.28434 (8)0.53033 (9)0.0471 (3)
O10.17552 (15)0.09743 (8)0.30526 (8)0.0640 (4)
O20.00108 (12)0.00677 (10)0.32939 (9)0.0681 (4)
O30.03302 (15)0.19581 (9)0.55383 (9)0.0731 (4)
O40.04980 (16)0.33927 (11)0.60232 (9)0.0835 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0443 (8)0.0454 (9)0.0345 (8)0.0005 (7)0.0086 (6)0.0038 (7)
C20.0622 (11)0.0518 (11)0.0466 (10)0.0106 (9)0.0099 (8)0.0023 (8)
C30.0915 (16)0.0431 (11)0.0566 (12)0.0016 (10)0.0041 (11)0.0093 (9)
C40.0788 (15)0.0715 (15)0.0575 (12)0.0225 (12)0.0011 (11)0.0207 (11)
C50.0568 (11)0.0875 (17)0.0642 (13)0.0109 (11)0.0197 (10)0.0173 (11)
C60.0516 (10)0.0572 (11)0.0527 (10)0.0033 (8)0.0190 (8)0.0081 (8)
C70.0428 (9)0.0455 (9)0.0535 (10)0.0049 (7)0.0141 (7)0.0040 (8)
C80.0537 (10)0.0494 (10)0.0440 (9)0.0010 (8)0.0031 (8)0.0001 (8)
C90.0548 (10)0.0393 (9)0.0406 (9)0.0002 (7)0.0128 (7)0.0005 (7)
C100.0441 (9)0.0697 (12)0.0467 (10)0.0065 (8)0.0187 (8)0.0031 (9)
C110.0517 (10)0.0731 (13)0.0529 (11)0.0179 (9)0.0126 (8)0.0005 (10)
C120.0562 (12)0.1058 (19)0.0498 (11)0.0274 (12)0.0103 (9)0.0004 (11)
C130.0538 (12)0.116 (2)0.0645 (14)0.0023 (13)0.0175 (10)0.0288 (14)
C140.0756 (15)0.0935 (18)0.0827 (17)0.0225 (13)0.0353 (13)0.0278 (14)
C150.0696 (13)0.0773 (15)0.0645 (13)0.0066 (11)0.0302 (11)0.0013 (11)
C160.0457 (9)0.0525 (10)0.0452 (9)0.0054 (7)0.0194 (7)0.0055 (8)
C170.0541 (10)0.0451 (10)0.0562 (11)0.0058 (8)0.0251 (8)0.0056 (8)
C180.0438 (9)0.0475 (10)0.0630 (11)0.0008 (7)0.0202 (8)0.0158 (8)
C190.0620 (12)0.0681 (14)0.1120 (18)0.0155 (10)0.0332 (12)0.0454 (13)
C200.0659 (12)0.0840 (15)0.0531 (11)0.0020 (11)0.0097 (10)0.0099 (10)
C210.0589 (11)0.0413 (10)0.0753 (13)0.0053 (8)0.0156 (10)0.0067 (9)
C220.0615 (11)0.0498 (11)0.0531 (11)0.0114 (9)0.0087 (9)0.0063 (8)
C230.0587 (11)0.0406 (9)0.0563 (11)0.0075 (8)0.0118 (9)0.0039 (8)
C240.0613 (13)0.0879 (16)0.0791 (15)0.0081 (11)0.0149 (11)0.0044 (12)
C250.0820 (14)0.0602 (13)0.0629 (12)0.0052 (10)0.0213 (11)0.0020 (10)
S10.0477 (2)0.0487 (3)0.0404 (2)0.00946 (18)0.01282 (18)0.00255 (18)
S20.0538 (3)0.0726 (3)0.0396 (2)0.0046 (2)0.01724 (19)0.0030 (2)
N10.0468 (7)0.0399 (7)0.0391 (7)0.0034 (6)0.0154 (6)0.0006 (6)
N20.0496 (8)0.0396 (8)0.0514 (8)0.0048 (6)0.0150 (6)0.0080 (6)
O10.0970 (10)0.0473 (7)0.0508 (7)0.0128 (7)0.0278 (7)0.0122 (6)
O20.0410 (7)0.0977 (11)0.0602 (8)0.0125 (7)0.0085 (6)0.0028 (7)
O30.0737 (9)0.0857 (10)0.0600 (8)0.0195 (8)0.0212 (7)0.0211 (7)
O40.0794 (10)0.1212 (13)0.0523 (8)0.0133 (9)0.0240 (7)0.0253 (8)
Geometric parameters (Å, º) top
C1—C61.381 (2)C16—N11.479 (2)
C1—C21.382 (2)C16—C171.494 (2)
C1—S11.7651 (16)C16—H16A0.9700
C2—C31.382 (3)C16—H16B0.9700
C2—H20.9300C17—C181.315 (2)
C3—C41.371 (3)C17—H170.9300
C3—H30.9300C18—C201.495 (3)
C4—C51.365 (3)C18—C191.496 (3)
C4—H40.9300C19—H19A0.9600
C5—C61.381 (3)C19—H19B0.9600
C5—H50.9300C19—H19C0.9600
C6—H60.9300C20—H20A0.9600
C7—N11.469 (2)C20—H20B0.9600
C7—C81.515 (2)C20—H20C0.9600
C7—H7A0.9700C21—N21.482 (2)
C7—H7B0.9700C21—C221.494 (3)
C8—C91.512 (2)C21—H21A0.9700
C8—H8A0.9700C21—H21B0.9700
C8—H8B0.9700C22—C231.318 (3)
C9—N21.476 (2)C22—H220.9300
C9—H9A0.9700C23—C251.502 (3)
C9—H9B0.9700C23—C241.502 (3)
C10—C151.378 (3)C24—H24A0.9600
C10—C111.385 (3)C24—H24B0.9600
C10—S21.7719 (18)C24—H24C0.9600
C11—C121.390 (3)C25—H25A0.9600
C11—H110.9300C25—H25B0.9600
C12—C131.359 (3)C25—H25C0.9600
C12—H120.9300S1—O11.4284 (13)
C13—C141.363 (4)S1—O21.4284 (13)
C13—H130.9300S1—N11.6184 (13)
C14—C151.386 (3)S2—O41.4242 (15)
C14—H140.9300S2—O31.4270 (15)
C15—H150.9300S2—N21.6263 (14)
C6—C1—C2120.38 (16)C18—C17—C16126.79 (17)
C6—C1—S1119.91 (13)C18—C17—H17116.6
C2—C1—S1119.66 (13)C16—C17—H17116.6
C3—C2—C1119.10 (19)C17—C18—C20123.69 (17)
C3—C2—H2120.4C17—C18—C19121.47 (19)
C1—C2—H2120.4C20—C18—C19114.83 (18)
C4—C3—C2120.6 (2)C18—C19—H19A109.5
C4—C3—H3119.7C18—C19—H19B109.5
C2—C3—H3119.7H19A—C19—H19B109.5
C5—C4—C3120.01 (19)C18—C19—H19C109.5
C5—C4—H4120.0H19A—C19—H19C109.5
C3—C4—H4120.0H19B—C19—H19C109.5
C4—C5—C6120.5 (2)C18—C20—H20A109.5
C4—C5—H5119.7C18—C20—H20B109.5
C6—C5—H5119.7H20A—C20—H20B109.5
C1—C6—C5119.36 (18)C18—C20—H20C109.5
C1—C6—H6120.3H20A—C20—H20C109.5
C5—C6—H6120.3H20B—C20—H20C109.5
N1—C7—C8111.98 (13)N2—C21—C22111.09 (15)
N1—C7—H7A109.2N2—C21—H21A109.4
C8—C7—H7A109.2C22—C21—H21A109.4
N1—C7—H7B109.2N2—C21—H21B109.4
C8—C7—H7B109.2C22—C21—H21B109.4
H7A—C7—H7B107.9H21A—C21—H21B108.0
C9—C8—C7112.71 (14)C23—C22—C21127.35 (19)
C9—C8—H8A109.1C23—C22—H22116.3
C7—C8—H8A109.1C21—C22—H22116.3
C9—C8—H8B109.1C22—C23—C25125.31 (18)
C7—C8—H8B109.1C22—C23—C24120.94 (19)
H8A—C8—H8B107.8C25—C23—C24113.74 (18)
N2—C9—C8113.03 (14)C23—C24—H24A109.5
N2—C9—H9A109.0C23—C24—H24B109.5
C8—C9—H9A109.0H24A—C24—H24B109.5
N2—C9—H9B109.0C23—C24—H24C109.5
C8—C9—H9B109.0H24A—C24—H24C109.5
H9A—C9—H9B107.8H24B—C24—H24C109.5
C15—C10—C11120.45 (19)C23—C25—H25A109.5
C15—C10—S2119.67 (15)C23—C25—H25B109.5
C11—C10—S2119.88 (16)H25A—C25—H25B109.5
C10—C11—C12118.6 (2)C23—C25—H25C109.5
C10—C11—H11120.7H25A—C25—H25C109.5
C12—C11—H11120.7H25B—C25—H25C109.5
C13—C12—C11120.8 (2)O1—S1—O2119.91 (9)
C13—C12—H12119.6O1—S1—N1106.84 (8)
C11—C12—H12119.6O2—S1—N1107.44 (7)
C12—C13—C14120.4 (2)O1—S1—C1107.54 (8)
C12—C13—H13119.8O2—S1—C1107.08 (8)
C14—C13—H13119.8N1—S1—C1107.48 (7)
C13—C14—C15120.3 (2)O4—S2—O3119.78 (10)
C13—C14—H14119.8O4—S2—N2107.31 (8)
C15—C14—H14119.8O3—S2—N2106.30 (8)
C10—C15—C14119.4 (2)O4—S2—C10107.05 (10)
C10—C15—H15120.3O3—S2—C10108.20 (9)
C14—C15—H15120.3N2—S2—C10107.68 (8)
N1—C16—C17113.23 (13)C7—N1—C16116.35 (13)
N1—C16—H16A108.9C7—N1—S1120.42 (11)
C17—C16—H16A108.9C16—N1—S1119.30 (11)
N1—C16—H16B108.9C9—N2—C21115.59 (14)
C17—C16—H16B108.9C9—N2—S2116.26 (11)
H16A—C16—H16B107.7C21—N2—S2117.54 (12)
C6—C1—C2—C31.1 (3)C6—C1—S1—N192.54 (15)
S1—C1—C2—C3176.26 (14)C2—C1—S1—N184.80 (15)
C1—C2—C3—C40.7 (3)C15—C10—S2—O417.51 (18)
C2—C3—C4—C50.2 (3)C11—C10—S2—O4163.10 (14)
C3—C4—C5—C60.7 (3)C15—C10—S2—O3147.88 (15)
C2—C1—C6—C50.6 (3)C11—C10—S2—O332.73 (16)
S1—C1—C6—C5176.70 (14)C15—C10—S2—N297.60 (15)
C4—C5—C6—C10.2 (3)C11—C10—S2—N281.79 (15)
N1—C7—C8—C968.49 (19)C8—C7—N1—C1685.97 (17)
C7—C8—C9—N2167.95 (14)C8—C7—N1—S1116.52 (14)
C15—C10—C11—C121.2 (3)C17—C16—N1—C757.52 (19)
S2—C10—C11—C12178.17 (14)C17—C16—N1—S1100.26 (15)
C10—C11—C12—C131.9 (3)O1—S1—N1—C731.34 (14)
C11—C12—C13—C141.0 (3)O2—S1—N1—C7161.22 (12)
C12—C13—C14—C150.5 (3)C1—S1—N1—C783.85 (13)
C11—C10—C15—C140.3 (3)O1—S1—N1—C16171.81 (11)
S2—C10—C15—C14179.66 (15)O2—S1—N1—C1641.93 (13)
C13—C14—C15—C101.2 (3)C1—S1—N1—C1673.01 (13)
N1—C16—C17—C18121.44 (18)C8—C9—N2—C21117.43 (17)
C16—C17—C18—C200.9 (3)C8—C9—N2—S298.69 (16)
C16—C17—C18—C19177.71 (17)C22—C21—N2—C968.0 (2)
N2—C21—C22—C23117.5 (2)C22—C21—N2—S2148.57 (14)
C21—C22—C23—C251.5 (3)O4—S2—N2—C9170.32 (12)
C21—C22—C23—C24177.22 (19)O3—S2—N2—C941.04 (14)
C6—C1—S1—O122.18 (16)C10—S2—N2—C974.74 (14)
C2—C1—S1—O1160.49 (14)O4—S2—N2—C2146.52 (16)
C6—C1—S1—O2152.29 (14)O3—S2—N2—C21175.80 (13)
C2—C1—S1—O230.38 (16)C10—S2—N2—C2168.42 (15)

Experimental details

Crystal data
Chemical formulaC25H34N2O4S2
Mr490.66
Crystal system, space groupMonoclinic, P21/n
Temperature (K)296
a, b, c (Å)10.3019 (2), 16.3962 (4), 16.0500 (4)
β (°) 108.449 (1)
V3)2571.71 (10)
Z4
Radiation typeMo Kα
µ (mm1)0.24
Crystal size (mm)0.50 × 0.25 × 0.20
Data collection
DiffractometerBruker APEXII CCD
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
40701, 5059, 4011
Rint0.028
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.034, 0.102, 1.05
No. of reflections5059
No. of parameters302
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.25, 0.24

Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997).

 

Acknowledgements

IUK thanks the Higher Education Commission of Pakistan for its financial support under the project to strengthe the Materials Chemistry Laboratory at GCUL.

References

First citationBruker (2007). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationFarrugia, L. J. (1997). J. Appl. Cryst. 30, 565.  CrossRef IUCr Journals Google Scholar
First citationKhan, I. U., Sheikh, T. A., Ejaz, & Harrison, W. T. A. (2011). Acta Cryst. E67, o2371.  Google Scholar
First citationSheikh, T. A., Khan, I. U., Harrison, W. T. A. & Ejaz, (2011). Acta Cryst. E67, o1737.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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