Abstract
The title compound, C9H8Br2N2O3, is planar (r.m.s. deviation = 0.030 Å) with the exception of the terminal methyl group which lies out of the plane [1.219 (3) Å]. The conformation about the C=N double bond [1.268 (3) Å] is E. An intramolecular N—H⋯N hydrogen bond occurs. Linear supramolecular chains along the b axis mediated by O—H⋯O hydrogen-bonding interactions feature in the crystal structure. These chains are also stabilized by weak C—H⋯N contacts.
Related literature
For the preparation of isonitrosoacetanilides from aniline derivatives, see: Garden et al. (1997 ▶). For the use of isonitrosoacetanilides as precursors of pharmacologically important heterocyclic compounds, see: da Silva et al. (2001 ▶); Garden et al. (2002 ▶); Matheus et al. (2007 ▶); Maronas et al. (2008 ▶). For related structures, see: Briansó et al. (1974 ▶); Plana et al. (1976 ▶).
Experimental
Crystal data
C9H8Br2N2O3
M r = 351.98
Monoclinic,
a = 10.3841 (2) Å
b = 8.8535 (1) Å
c = 13.0164 (3) Å
β = 106.356 (1)°
V = 1148.24 (4) Å3
Z = 4
Mo Kα radiation
μ = 7.05 mm−1
T = 120 K
0.20 × 0.10 × 0.01 mm
Data collection
Nonius KappaCCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 2007 ▶) T min = 0.715, T max = 1.000
14309 measured reflections
2643 independent reflections
2306 reflections with I > 2σ(I)
R int = 0.036
Refinement
R[F 2 > 2σ(F 2)] = 0.028
wR(F 2) = 0.090
S = 1.16
2643 reflections
149 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.77 e Å−3
Δρmin = −0.86 e Å−3
Data collection: COLLECT (Hooft, 1998 ▶); cell refinement: DENZO (Otwinowski & Minor, 1997 ▶) and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810018623/hg2689sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810018623/hg2689Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1n⋯N2 | 0.88 | 2.30 | 2.702 (3) | 108 |
| O2—H2o⋯O1i | 0.84 | 1.83 | 2.672 (3) | 175 |
| C2—H2⋯N2ii | 0.95 | 2.51 | 3.345 (3) | 146 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The use of the EPSRC X-ray crystallographic service at the University of Southampton, England, and the valuable assistance of the staff there is gratefully acknowledged. SJG thanks CNPq and FAPERJ for financial support.
supplementary crystallographic information
Comment
Isonitrosoacetanilides, readily available from aniline derivatives (Garden et al., 1997), have found use as precursors of pharmacologically important heterocyclic compounds (da Silva et al., 2001; Garden et al., 2002; Matheus et al., 2007; Maronas et al., 2008).
The molecular structure of (I), Fig. 1, is essentially planar with the exception of the terminal methyl group. Thus, the r.m.s. deviation of all non-hydrogen atoms, excluding the methyl-C9 atom, is 0.030 Å; the C9 atom lies 1.219 (3) Å out of the plane. The conformation about the C2═N2 double bond [1.268 (3) Å] is E. The observed planarity is partially stabilised by an intramolecular N–H···N hydrogen bond (Table 1). There two other methoxy substituted 2-(hydroxyimino)-N-arylacetamide structures available for comparison,i.e. o-OMe (Plana et al., 1976) and p-OMe (Briansó et al., 1974) derivatives. The geometric parameters in these match closely those in (I). The major difference in the three structures relate to the non-planarity of (I) compared to the planarity in the literature structures. The proximity of the OMe group to two bromido substituents in (I) is the likely explanation for the deviation from planarity in (I). The crystal packing is dominated by O–H···O hydrogen bonding interactions that lead to the formation of a supramolecular linear chain along the b axis, Fig. 2 and Table 1. These chains are also stabilised by weak C–H···N contacts, Table 1.
Experimental
The compound was prepared as previously reported from 3,5-dibromo-4-methoxyaniline, hydroxylamine.hydrogen sulfate in aqueous ethanol, containing sodium sulfate and CCl3CH(OH)2 (Garden et al., 1997). The sample for the crystallographic study was recrystallised from EtOH, m.p. 463 K.
Refinement
The O-, N- and C-bound H atoms were geometrically placed (O–H = 0.84 Å, N–H = 0.88 Å and C–H = 0.95–0.98 Å) and refined as riding with Uiso(H) = 1.2-1.5Ueq(parent atom).
Figures
Fig. 1.
The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of a supramolecular array in (I) aligned along the b axis. The O–H···O hydrogen bonding interactions are shown as orange dashed lines. Colour code: Br, olive; O, red; N, blue; C, grey; and H, green.
Crystal data
| C9H8Br2N2O3 | F(000) = 680 |
| Mr = 351.98 | Dx = 2.036 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 2760 reflections |
| a = 10.3841 (2) Å | θ = 2.9–27.5° |
| b = 8.8535 (1) Å | µ = 7.05 mm−1 |
| c = 13.0164 (3) Å | T = 120 K |
| β = 106.356 (1)° | Plate, colourless |
| V = 1148.24 (4) Å3 | 0.20 × 0.10 × 0.01 mm |
| Z = 4 |
Data collection
| Nonius KappaCCD area-detector diffractometer | 2643 independent reflections |
| Radiation source: Enraf Nonius FR591 rotating anode | 2306 reflections with I > 2σ(I) |
| 10 cm confocal mirrors | Rint = 0.036 |
| Detector resolution: 9.091 pixels mm-1 | θmax = 27.5°, θmin = 3.0° |
| φ and ω scans | h = −13→13 |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2007) | k = −11→10 |
| Tmin = 0.715, Tmax = 1.000 | l = −16→16 |
| 14309 measured reflections |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.090 | H-atom parameters constrained |
| S = 1.16 | w = 1/[σ2(Fo2) + (0.0554P)2 + 0.0437P] where P = (Fo2 + 2Fc2)/3 |
| 2643 reflections | (Δ/σ)max = 0.001 |
| 149 parameters | Δρmax = 0.77 e Å−3 |
| 1 restraint | Δρmin = −0.86 e Å−3 |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| Br1 | 0.51024 (3) | 0.51328 (3) | 0.64286 (2) | 0.03073 (12) | |
| Br2 | 0.57429 (3) | 1.12760 (3) | 0.76735 (2) | 0.03212 (12) | |
| O1 | 0.6650 (2) | 0.4317 (2) | 1.04372 (14) | 0.0253 (4) | |
| O2 | 0.7998 (2) | 0.6540 (2) | 1.37265 (15) | 0.0268 (4) | |
| H2O | 0.8150 | 0.7416 | 1.3979 | 0.040* | |
| O3 | 0.50326 (19) | 0.8555 (2) | 0.61613 (15) | 0.0248 (4) | |
| N2 | 0.7577 (2) | 0.6746 (2) | 1.26323 (17) | 0.0228 (5) | |
| N1 | 0.6742 (2) | 0.6890 (2) | 1.04718 (16) | 0.0234 (5) | |
| H1N | 0.6916 | 0.7664 | 1.0914 | 0.028* | |
| C1 | 0.6888 (3) | 0.5517 (3) | 1.0935 (2) | 0.0216 (5) | |
| C2 | 0.7347 (3) | 0.5508 (3) | 1.2123 (2) | 0.0235 (5) | |
| H2 | 0.7469 | 0.4577 | 1.2501 | 0.028* | |
| C3 | 0.6344 (3) | 0.7255 (3) | 0.9367 (2) | 0.0217 (5) | |
| C4 | 0.5979 (3) | 0.6159 (3) | 0.8574 (2) | 0.0221 (5) | |
| H4 | 0.5995 | 0.5118 | 0.8755 | 0.027* | |
| C5 | 0.5590 (3) | 0.6618 (3) | 0.7514 (2) | 0.0218 (5) | |
| C6 | 0.5517 (2) | 0.8133 (3) | 0.7211 (2) | 0.0221 (5) | |
| C7 | 0.5887 (3) | 0.9197 (3) | 0.8032 (2) | 0.0238 (5) | |
| C8 | 0.6305 (3) | 0.8778 (3) | 0.9101 (2) | 0.0242 (6) | |
| H8 | 0.6562 | 0.9524 | 0.9645 | 0.029* | |
| C9 | 0.6056 (3) | 0.8606 (4) | 0.5605 (2) | 0.0332 (6) | |
| H9A | 0.6683 | 0.9431 | 0.5894 | 0.050* | |
| H9B | 0.5635 | 0.8776 | 0.4840 | 0.050* | |
| H9C | 0.6544 | 0.7645 | 0.5704 | 0.050* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.0466 (2) | 0.02593 (18) | 0.01798 (18) | −0.00608 (11) | 0.00633 (13) | −0.00244 (9) |
| Br2 | 0.0420 (2) | 0.01905 (17) | 0.0298 (2) | −0.00089 (10) | 0.00100 (13) | 0.00607 (10) |
| O1 | 0.0388 (11) | 0.0189 (9) | 0.0175 (9) | −0.0002 (8) | 0.0067 (8) | 0.0009 (7) |
| O2 | 0.0400 (11) | 0.0222 (9) | 0.0154 (9) | −0.0022 (8) | 0.0033 (8) | 0.0001 (7) |
| O3 | 0.0255 (9) | 0.0305 (10) | 0.0166 (9) | −0.0010 (7) | 0.0031 (7) | 0.0081 (7) |
| N2 | 0.0274 (12) | 0.0235 (11) | 0.0159 (11) | −0.0009 (8) | 0.0033 (8) | 0.0000 (8) |
| N1 | 0.0321 (12) | 0.0184 (10) | 0.0165 (11) | −0.0005 (9) | 0.0015 (9) | 0.0004 (8) |
| C1 | 0.0235 (12) | 0.0220 (12) | 0.0181 (13) | −0.0011 (10) | 0.0042 (10) | 0.0000 (10) |
| C2 | 0.0307 (14) | 0.0196 (12) | 0.0193 (13) | −0.0001 (10) | 0.0054 (10) | 0.0011 (10) |
| C3 | 0.0243 (12) | 0.0209 (12) | 0.0190 (13) | 0.0013 (10) | 0.0046 (10) | 0.0015 (9) |
| C4 | 0.0246 (13) | 0.0197 (12) | 0.0215 (14) | 0.0008 (9) | 0.0056 (10) | 0.0028 (9) |
| C5 | 0.0214 (12) | 0.0250 (12) | 0.0184 (13) | −0.0019 (10) | 0.0045 (10) | −0.0018 (10) |
| C6 | 0.0188 (12) | 0.0261 (13) | 0.0195 (13) | 0.0009 (10) | 0.0022 (10) | 0.0053 (10) |
| C7 | 0.0255 (13) | 0.0184 (12) | 0.0248 (14) | −0.0010 (10) | 0.0028 (10) | 0.0060 (10) |
| C8 | 0.0267 (13) | 0.0244 (13) | 0.0189 (13) | −0.0024 (10) | 0.0024 (10) | 0.0001 (9) |
| C9 | 0.0345 (16) | 0.0420 (16) | 0.0244 (15) | 0.0030 (12) | 0.0103 (12) | 0.0102 (12) |
Geometric parameters (Å, °)
| Br1—C5 | 1.892 (3) | C2—H2 | 0.9500 |
| Br2—C7 | 1.894 (3) | C3—C4 | 1.390 (4) |
| O1—C1 | 1.233 (3) | C3—C8 | 1.390 (4) |
| O2—N2 | 1.379 (3) | C4—C5 | 1.385 (3) |
| O2—H2o | 0.8400 | C4—H4 | 0.9500 |
| O3—C6 | 1.368 (3) | C5—C6 | 1.394 (4) |
| O3—C9 | 1.445 (3) | C6—C7 | 1.395 (4) |
| N2—C2 | 1.268 (3) | C7—C8 | 1.386 (4) |
| N1—C1 | 1.346 (3) | C8—H8 | 0.9500 |
| N1—C3 | 1.417 (3) | C9—H9A | 0.9800 |
| N1—H1N | 0.8800 | C9—H9B | 0.9800 |
| C1—C2 | 1.484 (4) | C9—H9C | 0.9800 |
| N2—O2—H2o | 104.6 | C4—C5—C6 | 122.8 (2) |
| C6—O3—C9 | 113.1 (2) | C4—C5—Br1 | 118.79 (19) |
| C2—N2—O2 | 112.6 (2) | C6—C5—Br1 | 118.39 (19) |
| C1—N1—C3 | 128.6 (2) | O3—C6—C5 | 121.4 (2) |
| C1—N1—H1N | 115.7 | O3—C6—C7 | 121.7 (2) |
| C3—N1—H1N | 115.7 | C5—C6—C7 | 116.8 (2) |
| O1—C1—N1 | 124.3 (2) | C8—C7—C6 | 121.9 (2) |
| O1—C1—C2 | 120.1 (2) | C8—C7—Br2 | 119.2 (2) |
| N1—C1—C2 | 115.7 (2) | C6—C7—Br2 | 118.81 (19) |
| N2—C2—C1 | 119.9 (2) | C7—C8—C3 | 119.3 (2) |
| N2—C2—H2 | 120.0 | C7—C8—H8 | 120.4 |
| C1—C2—H2 | 120.0 | C3—C8—H8 | 120.4 |
| C4—C3—C8 | 120.6 (2) | O3—C9—H9A | 109.5 |
| C4—C3—N1 | 122.4 (2) | O3—C9—H9B | 109.5 |
| C8—C3—N1 | 117.0 (2) | H9A—C9—H9B | 109.5 |
| C5—C4—C3 | 118.5 (2) | O3—C9—H9C | 109.5 |
| C5—C4—H4 | 120.7 | H9A—C9—H9C | 109.5 |
| C3—C4—H4 | 120.7 | H9B—C9—H9C | 109.5 |
| C3—N1—C1—O1 | −2.1 (4) | C4—C5—C6—O3 | −175.0 (2) |
| C3—N1—C1—C2 | 178.9 (2) | Br1—C5—C6—O3 | 3.8 (3) |
| O2—N2—C2—C1 | −179.9 (2) | C4—C5—C6—C7 | 1.3 (4) |
| O1—C1—C2—N2 | −179.2 (3) | Br1—C5—C6—C7 | −179.86 (19) |
| N1—C1—C2—N2 | −0.2 (4) | O3—C6—C7—C8 | 176.2 (2) |
| C1—N1—C3—C4 | 2.9 (4) | C5—C6—C7—C8 | −0.1 (4) |
| C1—N1—C3—C8 | −178.4 (3) | O3—C6—C7—Br2 | −1.3 (4) |
| C8—C3—C4—C5 | 0.7 (4) | C5—C6—C7—Br2 | −177.56 (18) |
| N1—C3—C4—C5 | 179.3 (2) | C6—C7—C8—C3 | −0.8 (4) |
| C3—C4—C5—C6 | −1.7 (4) | Br2—C7—C8—C3 | 176.7 (2) |
| C3—C4—C5—Br1 | 179.57 (19) | C4—C3—C8—C7 | 0.5 (4) |
| C9—O3—C6—C5 | −88.4 (3) | N1—C3—C8—C7 | −178.2 (2) |
| C9—O3—C6—C7 | 95.4 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1n···N2 | 0.88 | 2.30 | 2.702 (3) | 108 |
| O2—H2o···O1i | 0.84 | 1.83 | 2.672 (3) | 175 |
| C2—H2···N2ii | 0.95 | 2.51 | 3.345 (3) | 146 |
Symmetry codes: (i) −x+3/2, y+1/2, −z+5/2; (ii) −x+3/2, y−1/2, −z+5/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG2689).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810018623/hg2689sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810018623/hg2689Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


