supplementary materials


lh2490 scheme

Acta Cryst. (2007). E63, o4050    [ doi:10.1107/S160053680704398X ]

2-Methoxy-5-nitrobenzene-1,3-diyl bis(benzenesulfonate)

Z.-P. Xiao, R.-Q. Fang, H.-Q. Li and H.-L. Zhu

Abstract top

In the title molecule, C19H15NO9S2, the dihedral angle between the nitro group and the benzene ring to which it is attached is 11.68 (8)°. The N-C bond length of 1.466 (3) Å indicates that no conjugation exists between the nitro group and the benzene ring.

Comment top

Aromatic nitro compounds are potential intermediates for a variety of fine chemicals. They are easily reduced to the corresponding aromatic amines (Desai et al., 2001). Therefore, aromatic nitro compounds are frequently used in the synthesis of pharmaceuticals (Hoogenraad et al., 2004). We herein reported a crystal structure of 2-methoxy-5-nitrobenzene-1,3-diyl dibenzenesulfonate. As shown in Fig. 1, the nitro group (N1/O1/O2) makes a dihedral angle with the benzene ring (C1—C6) of 11.68 (8) °. In spite of the fact that the nitro group is almost coplanar with the benzene ring, no conjugation is observed as evidenced by the N1—C1 bond length of 1.466 (3) Å. This is an agreement with the standard values of single N—C bond (1.47–1.50 Å) and all other bonds distances are in the the normal ranges (Allen et al., 1987).

Related literature top

For related literature, see: Desai et al. (2001); Hoogenraad et al. (2004).

For bond-length data, see: Allen et al. (1987).

Experimental top

K2CO3 was charged into a solution of 2-hydroxy-5-nitrobenzene-1,3-diyl dibenzenesulfonate (4.66 g, 10 mmol) in anhydrous acetone (30 ml) with stirring. CH3I (0.66 ml, 13 mmol) was added dropwise to the reaction mixture at room temperature. The reaction mixture was then refluxed for 8 h. The residue was filtered and the cake washed with acetone. A shallow yellow solid was given in a yield of 85% after removal of the solvent. Recrystallization from acetone furnished volorless blocks for single-crystal structure determination.

Refinement top

All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C) and C—H = 0.93 Å for the aromatic H atoms or Uiso(H) = 1.5Ueq(C) and C—H = 0.96 Å for methyl H atoms.

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL (Sheldrick, 1997b).

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
2-Methoxy-5-nitrobenzene-1,3-diyl bis(benzenesulfonate) top
Crystal data top
C19H15NO9S2F000 = 960
Mr = 465.44Dx = 1.562 Mg m3
Monoclinic, P21/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 2407 reflections
a = 10.787 (2) Åθ = 1.3–25.4º
b = 10.895 (2) ŵ = 0.32 mm1
c = 16.876 (3) ÅT = 298 (2) K
β = 93.91 (3)ºBlock, colorless
V = 1978.7 (6) Å30.30 × 0.20 × 0.20 mm
Z = 4
Data collection top
Bruker SMART CCD
diffractometer
3872 independent reflections
Radiation source: fine-focus sealed tube2898 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.023
T = 298(2) Kθmax = 26.0º
φ and ω scansθmin = 1.9º
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
h = 0→13
Tmin = 0.909, Tmax = 0.938k = 0→13
4084 measured reflectionsl = 20→20
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.044  w = 1/[σ2(Fo2) + (0.0778P)2 + 0.2038P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.131(Δ/σ)max = 0.001
S = 1.05Δρmax = 0.40 e Å3
3872 reflectionsΔρmin = 0.33 e Å3
282 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.029 (2)
Secondary atom site location: difference Fourier map
Crystal data top
C19H15NO9S2V = 1978.7 (6) Å3
Mr = 465.44Z = 4
Monoclinic, P21/cMo Kα
a = 10.787 (2) ŵ = 0.32 mm1
b = 10.895 (2) ÅT = 298 (2) K
c = 16.876 (3) Å0.30 × 0.20 × 0.20 mm
β = 93.91 (3)º
Data collection top
Bruker SMART CCD
diffractometer
3872 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
2898 reflections with I > 2σ(I)
Tmin = 0.909, Tmax = 0.938Rint = 0.023
4084 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.044282 parameters
wR(F2) = 0.131H-atom parameters constrained
S = 1.05Δρmax = 0.40 e Å3
3872 reflectionsΔρmin = 0.33 e Å3
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 > 2sigma(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
S20.23217 (6)0.74187 (5)0.01047 (4)0.03603 (19)
S10.37812 (6)0.76657 (6)0.11612 (4)0.0407 (2)
O30.23769 (16)0.81284 (14)0.13794 (10)0.0410 (4)
O70.09188 (15)0.68927 (15)0.02396 (9)0.0404 (4)
O60.10742 (17)0.85730 (15)0.01565 (10)0.0461 (5)
O90.30660 (17)0.64741 (17)0.02568 (10)0.0515 (5)
O40.39210 (18)0.64822 (17)0.15073 (11)0.0524 (5)
O80.22762 (19)0.85748 (16)0.02797 (11)0.0559 (5)
O20.0900 (2)0.38064 (19)0.19229 (12)0.0659 (6)
O50.44911 (18)0.86750 (18)0.14039 (12)0.0596 (5)
C80.3875 (2)0.7536 (2)0.01236 (14)0.0377 (5)
C30.1401 (2)0.7322 (2)0.12367 (14)0.0354 (5)
C40.0728 (2)0.7565 (2)0.05757 (13)0.0347 (5)
C50.0243 (2)0.6747 (2)0.04417 (13)0.0355 (5)
C60.0520 (2)0.5758 (2)0.09344 (14)0.0379 (5)
H60.11440.52080.08230.046*
N10.0167 (2)0.4585 (2)0.21397 (14)0.0485 (5)
C140.2601 (2)0.7581 (2)0.11059 (14)0.0367 (5)
C20.1108 (2)0.6383 (2)0.17603 (14)0.0400 (6)
H20.15440.62760.22120.048*
C10.0152 (2)0.5605 (2)0.15972 (14)0.0383 (5)
C130.3827 (3)0.6383 (2)0.02110 (16)0.0499 (7)
H130.37570.56870.01080.060*
O10.0290 (2)0.4572 (2)0.27821 (13)0.0733 (7)
C90.3998 (3)0.8590 (3)0.03325 (17)0.0517 (7)
H90.40350.93580.00960.062*
C150.2564 (3)0.8751 (2)0.14369 (16)0.0486 (6)
H150.23770.94330.11360.058*
C190.2863 (3)0.6544 (3)0.15400 (16)0.0506 (7)
H190.28930.57720.13050.061*
C100.4065 (3)0.8469 (3)0.11472 (19)0.0673 (9)
H100.41510.91610.14690.081*
C70.0787 (3)0.8778 (3)0.06494 (15)0.0518 (7)
H7A0.00600.90440.06610.078*
H7B0.13290.93990.08820.078*
H7C0.09000.80290.09450.078*
C110.4003 (3)0.7318 (4)0.14827 (19)0.0696 (10)
H110.40420.72440.20330.084*
C170.3050 (3)0.7856 (4)0.26666 (18)0.0701 (10)
H170.31950.79480.32000.084*
C160.2811 (3)0.8871 (3)0.22228 (18)0.0628 (8)
H160.28160.96450.24540.075*
C180.3080 (3)0.6690 (3)0.23317 (17)0.0653 (9)
H180.32460.60090.26400.078*
C120.3885 (3)0.6280 (3)0.10238 (18)0.0689 (9)
H120.38440.55130.12610.083*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S20.0391 (3)0.0318 (3)0.0376 (3)0.0018 (2)0.0057 (2)0.0007 (2)
S10.0459 (4)0.0375 (4)0.0401 (4)0.0039 (3)0.0134 (3)0.0019 (3)
O30.0488 (10)0.0323 (9)0.0428 (9)0.0041 (8)0.0098 (8)0.0080 (7)
O70.0427 (9)0.0417 (10)0.0376 (9)0.0011 (8)0.0080 (7)0.0017 (8)
O60.0589 (11)0.0347 (9)0.0461 (10)0.0088 (8)0.0137 (8)0.0080 (8)
O90.0499 (11)0.0551 (12)0.0494 (10)0.0125 (9)0.0030 (8)0.0120 (9)
O40.0617 (12)0.0487 (11)0.0481 (10)0.0066 (9)0.0134 (9)0.0091 (9)
O80.0721 (13)0.0399 (10)0.0565 (11)0.0052 (9)0.0100 (10)0.0157 (9)
O20.0823 (15)0.0460 (12)0.0691 (14)0.0170 (11)0.0038 (11)0.0126 (10)
O50.0583 (12)0.0552 (12)0.0678 (12)0.0132 (10)0.0235 (10)0.0135 (10)
C80.0370 (12)0.0383 (13)0.0381 (13)0.0048 (10)0.0049 (10)0.0025 (10)
C30.0409 (13)0.0303 (12)0.0351 (12)0.0017 (10)0.0041 (10)0.0057 (10)
C40.0413 (13)0.0277 (12)0.0353 (12)0.0032 (10)0.0032 (10)0.0016 (9)
C50.0390 (13)0.0327 (12)0.0352 (12)0.0018 (10)0.0047 (10)0.0028 (10)
C60.0424 (13)0.0290 (12)0.0421 (13)0.0011 (10)0.0007 (10)0.0053 (10)
N10.0511 (13)0.0431 (13)0.0506 (13)0.0002 (11)0.0025 (10)0.0088 (11)
C140.0365 (12)0.0347 (13)0.0395 (13)0.0006 (10)0.0063 (10)0.0025 (10)
C20.0463 (14)0.0392 (14)0.0351 (12)0.0051 (11)0.0060 (10)0.0007 (10)
C10.0444 (13)0.0315 (12)0.0383 (13)0.0013 (10)0.0024 (10)0.0031 (10)
C130.0646 (18)0.0391 (14)0.0456 (15)0.0090 (13)0.0021 (13)0.0040 (12)
O10.0871 (16)0.0800 (16)0.0545 (12)0.0138 (13)0.0181 (11)0.0297 (12)
C90.0532 (16)0.0452 (16)0.0569 (16)0.0068 (13)0.0041 (13)0.0136 (13)
C150.0517 (16)0.0411 (15)0.0532 (15)0.0022 (12)0.0057 (12)0.0095 (12)
C190.0578 (17)0.0437 (15)0.0515 (16)0.0002 (13)0.0131 (13)0.0071 (12)
C100.0559 (18)0.083 (2)0.0621 (19)0.0016 (17)0.0033 (15)0.0365 (18)
C70.0597 (17)0.0515 (16)0.0451 (14)0.0122 (14)0.0096 (12)0.0128 (13)
C110.0580 (19)0.109 (3)0.0413 (16)0.0024 (19)0.0005 (14)0.0044 (18)
C170.0575 (19)0.115 (3)0.0375 (15)0.0043 (19)0.0043 (13)0.0124 (18)
C160.0611 (19)0.069 (2)0.0582 (18)0.0009 (16)0.0040 (15)0.0286 (16)
C180.069 (2)0.078 (2)0.0500 (17)0.0014 (18)0.0142 (15)0.0166 (16)
C120.083 (2)0.075 (2)0.0475 (17)0.0125 (19)0.0011 (16)0.0149 (16)
Geometric parameters (Å, °) top
S2—O91.4175 (18)C14—C151.391 (3)
S2—O81.4192 (18)C2—C11.377 (3)
S2—O71.6197 (18)C2—H20.9300
S2—C141.745 (2)C13—C121.374 (4)
S1—O51.4164 (19)C13—H130.9300
S1—O41.4278 (19)C9—C101.378 (4)
S1—O31.6150 (19)C9—H90.9300
S1—C81.753 (2)C15—C161.377 (4)
O3—C31.405 (3)C15—H150.9300
O7—C51.411 (3)C19—C181.381 (4)
O6—C41.345 (3)C19—H190.9300
O6—C71.433 (3)C10—C111.380 (5)
O2—N11.232 (3)C10—H100.9300
C8—C131.379 (3)C7—H7A0.9600
C8—C91.384 (3)C7—H7B0.9600
C3—C21.375 (3)C7—H7C0.9600
C3—C41.397 (3)C11—C121.371 (5)
C4—C51.406 (3)C11—H110.9300
C5—C61.381 (3)C17—C161.370 (5)
C6—C11.384 (3)C17—C181.390 (5)
C6—H60.9300C17—H170.9300
N1—O11.221 (3)C16—H160.9300
N1—C11.466 (3)C18—H180.9300
C14—C191.387 (3)C12—H120.9300
O9—S2—O8118.93 (12)C2—C1—C6121.9 (2)
O9—S2—O7107.45 (11)C2—C1—N1119.3 (2)
O8—S2—O7108.49 (11)C6—C1—N1118.9 (2)
O9—S2—C14111.12 (11)C12—C13—C8118.8 (3)
O8—S2—C14111.47 (12)C12—C13—H13120.6
O7—S2—C1496.97 (10)C8—C13—H13120.6
O5—S1—O4120.56 (12)C10—C9—C8118.2 (3)
O5—S1—O3102.05 (11)C10—C9—H9120.9
O4—S1—O3108.19 (11)C8—C9—H9120.9
O5—S1—C8110.87 (12)C16—C15—C14118.1 (3)
O4—S1—C8109.59 (11)C16—C15—H15120.9
O3—S1—C8104.02 (10)C14—C15—H15120.9
C3—O3—S1117.91 (14)C18—C19—C14118.1 (3)
C5—O7—S2117.04 (14)C18—C19—H19120.9
C4—O6—C7123.80 (19)C14—C19—H19120.9
C13—C8—C9122.2 (2)C9—C10—C11119.7 (3)
C13—C8—S1118.77 (19)C9—C10—H10120.2
C9—C8—S1119.0 (2)C11—C10—H10120.2
C2—C3—C4123.0 (2)O6—C7—H7A109.5
C2—C3—O3119.8 (2)O6—C7—H7B109.5
C4—C3—O3117.1 (2)H7A—C7—H7B109.5
O6—C4—C3115.7 (2)O6—C7—H7C109.5
O6—C4—C5128.0 (2)H7A—C7—H7C109.5
C3—C4—C5116.2 (2)H7B—C7—H7C109.5
C6—C5—C4122.0 (2)C12—C11—C10121.5 (3)
C6—C5—O7118.4 (2)C12—C11—H11119.2
C4—C5—O7119.4 (2)C10—C11—H11119.2
C5—C6—C1118.5 (2)C16—C17—C18121.0 (3)
C5—C6—H6120.7C16—C17—H17119.5
C1—C6—H6120.7C18—C17—H17119.5
O1—N1—O2124.2 (2)C17—C16—C15120.4 (3)
O1—N1—C1118.1 (2)C17—C16—H16119.8
O2—N1—C1117.7 (2)C15—C16—H16119.8
C19—C14—C15122.4 (2)C19—C18—C17119.8 (3)
C19—C14—S2118.91 (19)C19—C18—H18120.1
C15—C14—S2118.67 (19)C17—C18—H18120.1
C3—C2—C1118.2 (2)C11—C12—C13119.5 (3)
C3—C2—H2120.9C11—C12—H12120.2
C1—C2—H2120.9C13—C12—H12120.2
Acknowledgements top

The work was financed by grants (project 30672516) from the National Natural Science Foundation of China.

references
References top

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Hoogenraad, M., van der Linden, J. B. & Smith, A. A. (2004). Org. Process Res. Dev. 8, 469–476.

Sheldrick, G. M. (1997a). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Sheldrick, G. M. (1997b). SHELXTL. Bruker AXS Inc., Madison, Wisconsin, USA.