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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jul 5;64(Pt 8):o1410. doi: 10.1107/S1600536808019983

2,2,2-Trimethyl-N-(phenyl­sulfon­yl)­acetamide

B Thimme Gowda a,*, Sabine Foro b, B P Sowmya a, P G Nirmala a, Hartmut Fuess b
PMCID: PMC2962045  PMID: 21203130

Abstract

The N—H and C=O bonds of the SO2—NH—CO group in the title compound, C11H15NO3S, are anti to each other. The asymmetric unit contains two independent mol­ecules. The benzene rings form dihedral angles of 83.19 (8) and 76.01 (10)° with the mean planes of the C2NOS fragments. The mol­ecules are linked into chains parallel to the b axis by inter­molecular N—H⋯O hydrogen bonds.

Related literature

For related literature, see: Gowda, Nayak et al. (2007); Gowda, Foro & Fuess (2007); Gowda, Kožíšek et al. (2007); Gowda, Svoboda et al. (2007).graphic file with name e-64-o1410-scheme1.jpg

Experimental

Crystal data

  • C11H15NO3S

  • M r = 241.30

  • Monoclinic, Inline graphic

  • a = 12.3045 (9) Å

  • b = 11.3016 (7) Å

  • c = 18.466 (1) Å

  • β = 103.117 (6)°

  • V = 2500.9 (3) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.25 mm−1

  • T = 299 (2) K

  • 0.50 × 0.48 × 0.40 mm

Data collection

  • Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2007) T min = 0.885, T max = 0.906

  • 15589 measured reflections

  • 4985 independent reflections

  • 3639 reflections with I > 2σ(I)

  • R int = 0.029

Refinement

  • R[F 2 > 2σ(F 2)] = 0.051

  • wR(F 2) = 0.167

  • S = 1.16

  • 4985 reflections

  • 290 parameters

  • H-atom parameters constrained

  • Δρmax = 0.44 e Å−3

  • Δρmin = −0.40 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2007); cell refinement: CrysAlis RED (Oxford Diffraction, 2007); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808019983/rz2222sup1.cif

e-64-o1410-sup1.cif (23.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808019983/rz2222Isup2.hkl

e-64-o1410-Isup2.hkl (244.2KB, 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—H1N⋯O4i 0.86 2.09 2.946 (3) 171
N2—H2N⋯O2ii 0.86 2.32 3.094 (3) 151

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for extensions of his research fellowship.

supplementary crystallographic information

Comment

In the present work, as part of a study of the substituent effects on the solid state geometries of N-(aryl)-sulfonamides and substituted amides, the structure of N-(phenylsulfonyl)-2,2,2-trimethylacetamide (NPSTMAA) has been determined. The conformations of the N—H and C=O bonds of the SO2—NH—CO group in NPSTMAA are anti to each other (Fig. 1). The asymmetric unit of the structure contains two molecules. The bond parameters in NPSTMAA are similar to those in N-(aryl)-2,2,2-trimethylacetamides (Gowda, Foro & Fuess, 2007; Gowda, Kožíšek et al., 2007; Gowda, Svoboda et al., 2007) and benzenesulfonamide (Gowda, Nayak et al., 2007). The benzene rings form dihedral angles of 83.19 (8) and 76.01 (10)° with the mean planes of the C2NOS fragments. A packing diagram of NPSTMAA molecules showing the formation of molecular chains parallel to the b axis through N—H···O hydrogen bonds (Table 1) is shown in Fig. 2.

Experimental

The title compound was prepared by refluxing benzenesulfonamide (0.10 mol) in excess pivalyl chloride (0.20 mol) for about an hour on a water bath. The reaction mixture was cooled and poured into ice-cold water. The resulting solid was separated, washed thoroughly with water and dissolved in a warm sodium hydrogen carbonate solution. The title compound was precipitated by acidifying the filtered solution with glacial acetic acid. It was filtered, dried and recrystallized from ethanol. The purity of the compound was checked by determining its melting point. It was characterized by recording its infrared and NMR spectra. Single crystals of the title compound suitable for X-ray diffraction studies were obtained by slow evaporation of an ethanol solution.

Refinement

The H atoms were positioned with idealized geometry using a riding model with C—H = 0.93–0.96 Å, N—H = 0.86 Å, and were refined with isotropic displacement parameters set to 1.2 times of the Ueq of the parent atom.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing the atom labeling scheme and displacement ellipsoids drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

The molecular packing of the title compound viewed along tha a axis. Hydrogen bonds are shown as dashed lines.

Crystal data

C11H15NO3S F000 = 1024
Mr = 241.30 Dx = 1.282 Mg m3
Monoclinic, P21/c Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 7426 reflections
a = 12.3045 (9) Å θ = 2.5–28.0º
b = 11.3016 (7) Å µ = 0.25 mm1
c = 18.466 (1) Å T = 299 (2) K
β = 103.117 (6)º Prism, colourless
V = 2500.9 (3) Å3 0.50 × 0.48 × 0.40 mm
Z = 8

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector 4985 independent reflections
Radiation source: fine-focus sealed tube 3639 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.029
T = 299(2) K θmax = 26.4º
Rotation method data acquisition using ω and φ scans θmin = 2.5º
Absorption correction: multi-scan(CrysAlis RED; Oxford Diffraction, 2007) h = −15→15
Tmin = 0.885, Tmax = 0.906 k = −13→13
15589 measured reflections l = −21→22

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.051   w = 1/[σ2(Fo2) + (0.0676P)2 + 1.8991P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.167 (Δ/σ)max = 0.002
S = 1.16 Δρmax = 0.44 e Å3
4985 reflections Δρmin = −0.40 e Å3
290 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.100 (4)
Secondary atom site location: difference Fourier map

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
C1 0.6562 (2) 0.7079 (2) 0.00179 (14) 0.0448 (6)
C2 0.7702 (3) 0.7222 (3) 0.00846 (18) 0.0580 (8)
H2 0.8043 0.7948 0.0223 0.070*
C3 0.8318 (3) 0.6267 (3) −0.0058 (2) 0.0693 (9)
H3 0.9082 0.6350 −0.0015 0.083*
C4 0.7817 (3) 0.5195 (3) −0.02624 (19) 0.0679 (9)
H4 0.8244 0.4554 −0.0350 0.081*
C5 0.6688 (3) 0.5067 (3) −0.03380 (18) 0.0624 (8)
H5 0.6350 0.4344 −0.0486 0.075*
C6 0.6053 (3) 0.6003 (3) −0.01956 (16) 0.0515 (7)
H6 0.5289 0.5913 −0.0242 0.062*
C7 0.5886 (2) 0.7797 (2) 0.15920 (15) 0.0440 (6)
C8 0.6204 (3) 0.8245 (3) 0.23927 (15) 0.0541 (7)
C9 0.5795 (4) 0.7357 (4) 0.2886 (2) 0.0894 (13)
H9A 0.6138 0.6603 0.2849 0.107*
H9B 0.5000 0.7281 0.2730 0.107*
H9C 0.5990 0.7625 0.3393 0.107*
C10 0.5687 (3) 0.9456 (3) 0.24601 (19) 0.0713 (9)
H10A 0.4889 0.9399 0.2307 0.086*
H10B 0.5953 1.0013 0.2148 0.086*
H10C 0.5892 0.9718 0.2967 0.086*
C11 0.7482 (3) 0.8339 (4) 0.2623 (2) 0.0856 (12)
H11A 0.7740 0.8874 0.2295 0.103*
H11B 0.7805 0.7572 0.2596 0.103*
H11C 0.7698 0.8630 0.3124 0.103*
N1 0.6084 (2) 0.8572 (2) 0.10554 (12) 0.0499 (6)
H1N 0.6401 0.9236 0.1200 0.060*
O1 0.46068 (17) 0.79593 (19) −0.00518 (12) 0.0590 (6)
O2 0.6126 (2) 0.93176 (18) −0.01691 (11) 0.0613 (6)
O3 0.54943 (18) 0.68328 (17) 0.14170 (11) 0.0541 (5)
S1 0.57470 (6) 0.82976 (6) 0.01579 (4) 0.0467 (2)
C12 0.8299 (2) 0.2840 (2) 0.14176 (14) 0.0476 (6)
C13 0.9320 (3) 0.3399 (3) 0.15839 (18) 0.0678 (9)
H13 0.9972 0.2991 0.1572 0.081*
C14 0.9346 (6) 0.4580 (5) 0.1769 (2) 0.1085 (19)
H14 1.0028 0.4973 0.1888 0.130*
C15 0.8403 (8) 0.5176 (4) 0.1781 (3) 0.120 (2)
H15 0.8442 0.5975 0.1905 0.144*
C16 0.7397 (5) 0.4626 (4) 0.1615 (2) 0.0985 (16)
H16 0.6752 0.5051 0.1625 0.118*
C17 0.7324 (3) 0.3431 (3) 0.14311 (17) 0.0657 (9)
H17 0.6640 0.3042 0.1321 0.079*
C18 0.8663 (2) 0.1631 (3) −0.01406 (16) 0.0531 (7)
C19 0.8292 (3) 0.1401 (3) −0.09727 (16) 0.0547 (7)
C20 0.9144 (4) 0.1923 (4) −0.1351 (2) 0.0894 (13)
H20A 0.9856 0.1557 −0.1160 0.107*
H20B 0.9202 0.2759 −0.1258 0.107*
H20C 0.8918 0.1785 −0.1877 0.107*
C21 0.8234 (4) 0.0072 (4) −0.1109 (2) 0.0822 (11)
H21A 0.7707 −0.0273 −0.0859 0.099*
H21B 0.8957 −0.0271 −0.0921 0.099*
H21C 0.8002 −0.0079 −0.1633 0.099*
C22 0.7149 (4) 0.1925 (5) −0.1277 (2) 0.0991 (15)
H22A 0.7175 0.2764 −0.1193 0.119*
H22B 0.6622 0.1573 −0.1030 0.119*
H22C 0.6925 0.1771 −0.1801 0.119*
N2 0.7948 (2) 0.1235 (2) 0.02886 (12) 0.0541 (6)
H2N 0.7323 0.0925 0.0067 0.065*
O4 0.7261 (2) 0.0845 (2) 0.13953 (12) 0.0719 (7)
O5 0.9285 (2) 0.0813 (2) 0.15009 (14) 0.0811 (8)
O6 0.9519 (2) 0.2109 (3) 0.01479 (13) 0.0823 (8)
S2 0.82357 (6) 0.13285 (7) 0.12026 (4) 0.0512 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0553 (15) 0.0441 (14) 0.0354 (12) −0.0074 (12) 0.0111 (11) −0.0005 (10)
C2 0.0561 (17) 0.0525 (17) 0.0625 (18) −0.0116 (14) 0.0070 (14) 0.0000 (14)
C3 0.0572 (19) 0.076 (2) 0.077 (2) 0.0004 (17) 0.0198 (16) 0.0044 (18)
C4 0.081 (2) 0.061 (2) 0.068 (2) 0.0118 (17) 0.0315 (17) −0.0010 (16)
C5 0.082 (2) 0.0481 (17) 0.0640 (19) −0.0070 (15) 0.0306 (16) −0.0093 (14)
C6 0.0598 (17) 0.0494 (16) 0.0481 (15) −0.0122 (13) 0.0184 (12) −0.0038 (12)
C7 0.0478 (14) 0.0402 (14) 0.0453 (14) 0.0023 (11) 0.0132 (11) −0.0035 (11)
C8 0.0719 (19) 0.0524 (16) 0.0370 (14) −0.0026 (14) 0.0103 (13) −0.0038 (12)
C9 0.144 (4) 0.079 (3) 0.0471 (18) −0.019 (3) 0.027 (2) 0.0023 (17)
C10 0.092 (3) 0.067 (2) 0.0593 (19) 0.0040 (19) 0.0272 (18) −0.0160 (16)
C11 0.082 (3) 0.099 (3) 0.064 (2) 0.008 (2) −0.0068 (19) −0.011 (2)
N1 0.0684 (15) 0.0436 (12) 0.0376 (11) −0.0118 (11) 0.0119 (10) −0.0049 (9)
O1 0.0524 (12) 0.0616 (13) 0.0582 (12) 0.0000 (10) 0.0025 (9) −0.0063 (10)
O2 0.0892 (16) 0.0466 (11) 0.0499 (11) −0.0053 (11) 0.0195 (10) 0.0045 (9)
O3 0.0697 (13) 0.0420 (11) 0.0520 (11) −0.0059 (9) 0.0165 (9) −0.0025 (8)
S1 0.0585 (4) 0.0419 (4) 0.0387 (4) −0.0035 (3) 0.0088 (3) −0.0003 (3)
C12 0.0596 (17) 0.0470 (15) 0.0345 (13) −0.0036 (12) 0.0071 (11) −0.0018 (11)
C13 0.077 (2) 0.075 (2) 0.0491 (17) −0.0233 (18) 0.0108 (15) −0.0077 (15)
C14 0.172 (5) 0.084 (3) 0.068 (3) −0.066 (4) 0.023 (3) −0.021 (2)
C15 0.244 (8) 0.054 (3) 0.064 (3) −0.014 (4) 0.039 (4) −0.011 (2)
C16 0.164 (5) 0.078 (3) 0.057 (2) 0.056 (3) 0.031 (3) 0.005 (2)
C17 0.077 (2) 0.072 (2) 0.0467 (16) 0.0168 (17) 0.0098 (15) 0.0002 (15)
C18 0.0506 (16) 0.0640 (18) 0.0474 (16) −0.0065 (14) 0.0164 (12) −0.0095 (13)
C19 0.0563 (17) 0.0657 (19) 0.0445 (15) −0.0009 (14) 0.0164 (12) −0.0089 (13)
C20 0.111 (3) 0.112 (3) 0.053 (2) −0.033 (3) 0.036 (2) −0.012 (2)
C21 0.114 (3) 0.074 (2) 0.068 (2) −0.010 (2) 0.040 (2) −0.0204 (18)
C22 0.085 (3) 0.152 (4) 0.056 (2) 0.037 (3) 0.0070 (19) −0.008 (2)
N2 0.0570 (14) 0.0692 (16) 0.0382 (12) −0.0159 (12) 0.0152 (10) −0.0152 (11)
O4 0.0986 (18) 0.0684 (15) 0.0565 (13) −0.0316 (13) 0.0338 (12) −0.0093 (11)
O5 0.0916 (18) 0.0805 (17) 0.0672 (15) 0.0328 (14) 0.0099 (13) 0.0079 (13)
O6 0.0625 (14) 0.132 (2) 0.0541 (13) −0.0361 (15) 0.0165 (11) −0.0164 (14)
S2 0.0652 (5) 0.0477 (4) 0.0410 (4) −0.0019 (3) 0.0130 (3) −0.0016 (3)

Geometric parameters (Å, °)

C1—C6 1.384 (4) C12—C13 1.377 (4)
C1—C2 1.389 (4) C12—C17 1.378 (4)
C1—S1 1.757 (3) C12—S2 1.752 (3)
C2—C3 1.378 (5) C13—C14 1.376 (6)
C2—H2 0.9300 C13—H13 0.9300
C3—C4 1.373 (5) C14—C15 1.347 (8)
C3—H3 0.9300 C14—H14 0.9300
C4—C5 1.372 (5) C15—C16 1.357 (8)
C4—H4 0.9300 C15—H15 0.9300
C5—C6 1.375 (4) C16—C17 1.391 (6)
C5—H5 0.9300 C16—H16 0.9300
C6—H6 0.9300 C17—H17 0.9300
C7—O3 1.206 (3) C18—O6 1.195 (4)
C7—N1 1.384 (3) C18—N2 1.386 (4)
C7—C8 1.527 (4) C18—C19 1.523 (4)
C8—C9 1.516 (5) C19—C20 1.506 (5)
C8—C10 1.526 (5) C19—C22 1.512 (5)
C8—C11 1.536 (5) C19—C21 1.522 (5)
C9—H9A 0.9600 C20—H20A 0.9600
C9—H9B 0.9600 C20—H20B 0.9600
C9—H9C 0.9600 C20—H20C 0.9600
C10—H10A 0.9600 C21—H21A 0.9600
C10—H10B 0.9600 C21—H21B 0.9600
C10—H10C 0.9600 C21—H21C 0.9600
C11—H11A 0.9600 C22—H22A 0.9600
C11—H11B 0.9600 C22—H22B 0.9600
C11—H11C 0.9600 C22—H22C 0.9600
N1—S1 1.644 (2) N2—S2 1.647 (2)
N1—H1N 0.8600 N2—H2N 0.8600
O1—S1 1.421 (2) O4—S2 1.434 (2)
O2—S1 1.428 (2) O5—S2 1.410 (2)
C6—C1—C2 120.7 (3) C13—C12—C17 121.9 (3)
C6—C1—S1 119.6 (2) C13—C12—S2 119.3 (3)
C2—C1—S1 119.6 (2) C17—C12—S2 118.8 (2)
C3—C2—C1 118.7 (3) C14—C13—C12 118.0 (4)
C3—C2—H2 120.7 C14—C13—H13 121.0
C1—C2—H2 120.7 C12—C13—H13 121.0
C4—C3—C2 120.8 (3) C15—C14—C13 121.2 (5)
C4—C3—H3 119.6 C15—C14—H14 119.4
C2—C3—H3 119.6 C13—C14—H14 119.4
C5—C4—C3 120.1 (3) C14—C15—C16 120.9 (4)
C5—C4—H4 119.9 C14—C15—H15 119.6
C3—C4—H4 119.9 C16—C15—H15 119.6
C4—C5—C6 120.4 (3) C15—C16—C17 120.3 (5)
C4—C5—H5 119.8 C15—C16—H16 119.9
C6—C5—H5 119.8 C17—C16—H16 119.9
C5—C6—C1 119.4 (3) C12—C17—C16 117.8 (4)
C5—C6—H6 120.3 C12—C17—H17 121.1
C1—C6—H6 120.3 C16—C17—H17 121.1
O3—C7—N1 120.3 (2) O6—C18—N2 120.0 (3)
O3—C7—C8 123.9 (3) O6—C18—C19 124.0 (3)
N1—C7—C8 115.8 (2) N2—C18—C19 116.0 (2)
C9—C8—C10 110.1 (3) C20—C19—C22 111.2 (4)
C9—C8—C7 108.4 (3) C20—C19—C21 108.7 (3)
C10—C8—C7 110.9 (2) C22—C19—C21 108.7 (3)
C9—C8—C11 109.7 (3) C20—C19—C18 108.7 (3)
C10—C8—C11 109.6 (3) C22—C19—C18 110.4 (3)
C7—C8—C11 108.2 (3) C21—C19—C18 109.1 (3)
C8—C9—H9A 109.5 C19—C20—H20A 109.5
C8—C9—H9B 109.5 C19—C20—H20B 109.5
H9A—C9—H9B 109.5 H20A—C20—H20B 109.5
C8—C9—H9C 109.5 C19—C20—H20C 109.5
H9A—C9—H9C 109.5 H20A—C20—H20C 109.5
H9B—C9—H9C 109.5 H20B—C20—H20C 109.5
C8—C10—H10A 109.5 C19—C21—H21A 109.5
C8—C10—H10B 109.5 C19—C21—H21B 109.5
H10A—C10—H10B 109.5 H21A—C21—H21B 109.5
C8—C10—H10C 109.5 C19—C21—H21C 109.5
H10A—C10—H10C 109.5 H21A—C21—H21C 109.5
H10B—C10—H10C 109.5 H21B—C21—H21C 109.5
C8—C11—H11A 109.5 C19—C22—H22A 109.5
C8—C11—H11B 109.5 C19—C22—H22B 109.5
H11A—C11—H11B 109.5 H22A—C22—H22B 109.5
C8—C11—H11C 109.5 C19—C22—H22C 109.5
H11A—C11—H11C 109.5 H22A—C22—H22C 109.5
H11B—C11—H11C 109.5 H22B—C22—H22C 109.5
C7—N1—S1 123.86 (19) C18—N2—S2 123.3 (2)
C7—N1—H1N 118.1 C18—N2—H2N 118.4
S1—N1—H1N 118.1 S2—N2—H2N 118.4
O1—S1—O2 119.96 (14) O5—S2—O4 119.27 (17)
O1—S1—N1 109.45 (13) O5—S2—N2 109.80 (14)
O2—S1—N1 104.02 (12) O4—S2—N2 103.43 (13)
O1—S1—C1 108.08 (13) O5—S2—C12 108.93 (16)
O2—S1—C1 108.55 (13) O4—S2—C12 108.21 (14)
N1—S1—C1 105.93 (12) N2—S2—C12 106.43 (13)
C6—C1—C2—C3 −0.7 (4) C17—C12—C13—C14 0.2 (5)
S1—C1—C2—C3 −177.3 (3) S2—C12—C13—C14 −178.4 (3)
C1—C2—C3—C4 0.1 (5) C12—C13—C14—C15 −0.6 (6)
C2—C3—C4—C5 0.9 (5) C13—C14—C15—C16 0.4 (7)
C3—C4—C5—C6 −1.3 (5) C14—C15—C16—C17 0.2 (7)
C4—C5—C6—C1 0.6 (5) C13—C12—C17—C16 0.4 (5)
C2—C1—C6—C5 0.4 (4) S2—C12—C17—C16 179.0 (3)
S1—C1—C6—C5 177.0 (2) C15—C16—C17—C12 −0.6 (6)
O3—C7—C8—C9 −7.8 (4) O6—C18—C19—C20 −2.7 (5)
N1—C7—C8—C9 172.8 (3) N2—C18—C19—C20 178.1 (3)
O3—C7—C8—C10 −128.7 (3) O6—C18—C19—C22 −124.9 (4)
N1—C7—C8—C10 51.9 (4) N2—C18—C19—C22 56.0 (4)
O3—C7—C8—C11 111.1 (3) O6—C18—C19—C21 115.7 (4)
N1—C7—C8—C11 −68.3 (3) N2—C18—C19—C21 −63.4 (4)
O3—C7—N1—S1 3.8 (4) O6—C18—N2—S2 −2.9 (5)
C8—C7—N1—S1 −176.8 (2) C19—C18—N2—S2 176.2 (2)
C7—N1—S1—O1 51.8 (3) C18—N2—S2—O5 −53.0 (3)
C7—N1—S1—O2 −178.8 (2) C18—N2—S2—O4 178.7 (3)
C7—N1—S1—C1 −64.5 (3) C18—N2—S2—C12 64.7 (3)
C6—C1—S1—O1 −5.4 (3) C13—C12—S2—O5 22.0 (3)
C2—C1—S1—O1 171.3 (2) C17—C12—S2—O5 −156.6 (2)
C6—C1—S1—O2 −136.9 (2) C13—C12—S2—O4 153.0 (2)
C2—C1—S1—O2 39.7 (3) C17—C12—S2—O4 −25.5 (3)
C6—C1—S1—N1 111.9 (2) C13—C12—S2—N2 −96.4 (2)
C2—C1—S1—N1 −71.5 (3) C17—C12—S2—N2 85.1 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O4i 0.86 2.09 2.946 (3) 171
N2—H2N···O2ii 0.86 2.32 3.094 (3) 151

Symmetry codes: (i) x, y+1, z; (ii) x, y−1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2222).

References

  1. Gowda, B. T., Foro, S. & Fuess, H. (2007). Acta Cryst. E63, o2329–o2330.
  2. Gowda, B. T., Kožíšek, J., Tokarčík, M. & Fuess, H. (2007). Acta Cryst. E63, o2327–o2328.
  3. Gowda, B. T., Nayak, R., Kožíšek, J., Tokarčík, M. & Fuess, H. (2007). Acta Cryst. E63, o2967.
  4. Gowda, B. T., Svoboda, I., Paulus, H. & Fuess, H. (2007). Z. Naturforsch. Teil A, 62, 331–337.
  5. Oxford Diffraction (2007). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Abingdon, Oxfordshire, England.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.

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/S1600536808019983/rz2222sup1.cif

e-64-o1410-sup1.cif (23.2KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808019983/rz2222Isup2.hkl

e-64-o1410-Isup2.hkl (244.2KB, hkl)

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


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