organic compounds
5-Bromo-1H-indole-2,3-dione
aDepartment of Chemistry and Biochemistry, University of Massachusetts Dartmouth, 285 Old Westport Road, North Dartmouth, MA 02747, USA
*Correspondence e-mail: dmanke@umassd.edu
The title compound, C8H4BrNO2, has a single, almost planar, planar molecule in the with the non-H atoms having a mean deviation from planarity of 0.024 Å. In the crystal, N—H⋯O hydrogen bonds link the molecules into [001] C(4) chains. C—H⋯O interactions form [0-11] chains. These interactions combine to generate sheets along (100). No π–π interactions are observed in the structure.
Keywords: crystal structure; hydrogen bonding; isatins.
CCDC reference: 1450609
Structure description
Herein, we report the ), as part of a continuing study on halogenated isatins. The structure exhibits a near planar molecule with the non-hydrogen atoms possessing a mean deviation from planarity of 0.024 Å, with similar bond lengths and angles to those observed in isatin (Goldschmidt et al., 1950). The structure of other bromoisatins report short Br⋯O contacts (Huang et al., 2016; Turbitt et al., 2016), which are not observed in 5-bromoisatin. The structures of N-subsistuted derivatives of 5-bromoisatin have been reported (Kurkin et al., 2008; Maamri et al., 2012) with only one instance of a Br⋯O interaction being observed (Kharbach et al., 2015).
of 5-bromoisatin (Fig. 1In the crystals, the molecules form [001] C(4) chains through N1—H1⋯O1 hydrogen bonds (Table 1). C7—H7⋯O2 interactions form [01] chains. The combination of these two interactions results i sheets along (100). No π–π interactions are observed in the structure. The packing of the title compound indicating hydrogen bonding is shown in Fig. 2.
Synthesis and crystallization
A commercial sample (Matrix Scientific) of 5-bromo-1H-indole-2,3-dione was used for the crystallization. A sample suitable for single-crystal X-ray analysis was grown from the slow evaporation of its acetonitrile solution.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 1450609
https://doi.org/10.1107/S2414314616001772/ff4002sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314616001772/ff4002Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314616001772/ff4002Isup3.cml
Data collection: APEX2 (Bruker, 2014); cell
SAINT (Bruker, 2014); data reduction: SAINT (Bruker, 2014); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009) and publCIF (Westrip, 2010).C8H4BrNO2 | F(000) = 440 |
Mr = 226.03 | Dx = 2.036 Mg m−3 |
Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2c -2n | Cell parameters from 5354 reflections |
a = 25.1411 (18) Å | θ = 3.2–25.4° |
b = 5.6851 (4) Å | µ = 5.52 mm−1 |
c = 5.1593 (3) Å | T = 120 K |
V = 737.42 (9) Å3 | Block, orange |
Z = 4 | 0.2 × 0.12 × 0.1 mm |
Bruker D8 Venture CMOS diffractometer | 1334 independent reflections |
Radiation source: Mo | 1232 reflections with I > 2σ(I) |
TRIUMPH monochromator | Rint = 0.035 |
φ and ω scans | θmax = 25.4°, θmin = 3.2° |
Absorption correction: multi-scan (SADABS; Bruker, 2014) | h = −30→30 |
Tmin = 0.109, Tmax = 0.148 | k = −6→6 |
8877 measured reflections | l = −6→6 |
Refinement on F2 | Hydrogen site location: mixed |
Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
R[F2 > 2σ(F2)] = 0.025 | w = 1/[σ2(Fo2) + 1.6735P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.054 | (Δ/σ)max < 0.001 |
S = 1.12 | Δρmax = 0.45 e Å−3 |
1334 reflections | Δρmin = −0.79 e Å−3 |
113 parameters | Absolute structure: Refined as an inversion twin |
2 restraints | Absolute structure parameter: 0.02 (2) |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
Refinement. Refined as a 2-component inversion twin. |
x | y | z | Uiso*/Ueq | ||
Br1 | 0.26549 (2) | 0.64837 (9) | 0.99780 (18) | 0.02277 (16) | |
O1 | 0.50004 (16) | 0.2784 (7) | 0.1243 (9) | 0.0188 (9) | |
O2 | 0.42674 (16) | 0.6864 (6) | 0.1519 (8) | 0.0185 (9) | |
N1 | 0.45090 (16) | 0.1622 (7) | 0.4830 (18) | 0.0185 (10) | |
H1 | 0.4664 (18) | 0.028 (5) | 0.496 (19) | 0.022* | |
C1 | 0.4649 (2) | 0.3068 (9) | 0.2839 (11) | 0.0151 (12) | |
C2 | 0.4258 (2) | 0.5187 (9) | 0.2971 (12) | 0.0144 (12) | |
C3 | 0.38981 (18) | 0.4647 (8) | 0.5154 (17) | 0.0146 (11) | |
C4 | 0.3472 (2) | 0.5867 (10) | 0.6209 (12) | 0.0156 (12) | |
H4 | 0.3359 | 0.7335 | 0.5523 | 0.019* | |
C5 | 0.3218 (2) | 0.4844 (10) | 0.8311 (11) | 0.0148 (12) | |
C6 | 0.3381 (2) | 0.2689 (10) | 0.9336 (10) | 0.0151 (14) | |
H6 | 0.3195 | 0.2040 | 1.0771 | 0.018* | |
C7 | 0.3812 (2) | 0.1476 (11) | 0.8286 (11) | 0.0176 (13) | |
H7 | 0.3925 | 0.0011 | 0.8980 | 0.021* | |
C8 | 0.4068 (2) | 0.2485 (10) | 0.6199 (11) | 0.0138 (11) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0220 (3) | 0.0254 (3) | 0.0210 (3) | 0.0056 (2) | 0.0035 (5) | −0.0021 (5) |
O1 | 0.021 (2) | 0.016 (2) | 0.020 (2) | 0.0018 (17) | 0.0033 (18) | −0.0030 (17) |
O2 | 0.026 (2) | 0.012 (2) | 0.017 (2) | 0.0028 (17) | −0.0013 (18) | 0.0046 (18) |
N1 | 0.020 (2) | 0.0111 (19) | 0.024 (3) | 0.0047 (18) | −0.002 (4) | 0.003 (3) |
C1 | 0.018 (3) | 0.009 (3) | 0.018 (3) | 0.002 (2) | −0.003 (3) | −0.002 (2) |
C2 | 0.016 (3) | 0.013 (3) | 0.014 (3) | −0.001 (2) | −0.004 (2) | −0.003 (2) |
C3 | 0.017 (2) | 0.015 (2) | 0.012 (3) | 0.0009 (19) | −0.004 (4) | 0.004 (4) |
C4 | 0.018 (3) | 0.013 (3) | 0.016 (3) | 0.002 (2) | −0.006 (2) | −0.001 (2) |
C5 | 0.016 (3) | 0.019 (3) | 0.010 (3) | 0.001 (2) | 0.000 (2) | −0.004 (2) |
C6 | 0.020 (3) | 0.016 (3) | 0.009 (4) | −0.005 (2) | −0.002 (2) | 0.000 (2) |
C7 | 0.021 (3) | 0.014 (3) | 0.018 (3) | −0.001 (3) | −0.004 (2) | 0.004 (3) |
C8 | 0.017 (3) | 0.011 (3) | 0.013 (3) | 0.001 (2) | −0.004 (2) | −0.003 (3) |
Br1—C5 | 1.901 (5) | C3—C8 | 1.409 (8) |
O1—C1 | 1.219 (7) | C4—H4 | 0.9500 |
O2—C2 | 1.213 (7) | C4—C5 | 1.386 (8) |
N1—H1 | 0.858 (14) | C5—C6 | 1.396 (8) |
N1—C1 | 1.362 (9) | C6—H6 | 0.9500 |
N1—C8 | 1.403 (8) | C6—C7 | 1.394 (8) |
C1—C2 | 1.555 (7) | C7—H7 | 0.9500 |
C2—C3 | 1.478 (9) | C7—C8 | 1.380 (8) |
C3—C4 | 1.387 (8) | ||
C1—N1—H1 | 119 (6) | C5—C4—H4 | 121.5 |
C1—N1—C8 | 111.9 (4) | C4—C5—Br1 | 119.4 (4) |
C8—N1—H1 | 129 (5) | C4—C5—C6 | 122.0 (5) |
O1—C1—N1 | 128.1 (5) | C6—C5—Br1 | 118.5 (4) |
O1—C1—C2 | 126.2 (5) | C5—C6—H6 | 119.5 |
N1—C1—C2 | 105.8 (5) | C7—C6—C5 | 121.0 (5) |
O2—C2—C1 | 124.7 (5) | C7—C6—H6 | 119.5 |
O2—C2—C3 | 130.2 (5) | C6—C7—H7 | 121.3 |
C3—C2—C1 | 105.0 (4) | C8—C7—C6 | 117.4 (5) |
C4—C3—C2 | 132.0 (5) | C8—C7—H7 | 121.3 |
C4—C3—C8 | 121.3 (6) | N1—C8—C3 | 110.6 (5) |
C8—C3—C2 | 106.7 (5) | C7—C8—N1 | 128.1 (5) |
C3—C4—H4 | 121.5 | C7—C8—C3 | 121.3 (5) |
C5—C4—C3 | 116.9 (5) | ||
Br1—C5—C6—C7 | −176.2 (4) | C2—C3—C8—C7 | −180.0 (5) |
O1—C1—C2—O2 | −2.1 (9) | C3—C4—C5—Br1 | 176.7 (5) |
O1—C1—C2—C3 | 177.5 (6) | C3—C4—C5—C6 | 0.1 (8) |
O2—C2—C3—C4 | −0.6 (11) | C4—C3—C8—N1 | −179.0 (6) |
O2—C2—C3—C8 | −179.4 (6) | C4—C3—C8—C7 | 1.1 (9) |
N1—C1—C2—O2 | 178.7 (6) | C4—C5—C6—C7 | 0.4 (8) |
N1—C1—C2—C3 | −1.7 (6) | C5—C6—C7—C8 | −0.2 (8) |
C1—N1—C8—C3 | −1.2 (7) | C6—C7—C8—N1 | 179.6 (6) |
C1—N1—C8—C7 | 178.7 (6) | C6—C7—C8—C3 | −0.6 (8) |
C1—C2—C3—C4 | 179.9 (7) | C8—N1—C1—O1 | −177.4 (6) |
C1—C2—C3—C8 | 1.1 (6) | C8—N1—C1—C2 | 1.8 (7) |
C2—C3—C4—C5 | −179.5 (6) | C8—C3—C4—C5 | −0.8 (9) |
C2—C3—C8—N1 | −0.1 (7) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.86 (1) | 2.05 (3) | 2.886 (6) | 166 (9) |
C7—H7···O2ii | 0.95 | 2.38 | 3.312 (7) | 167 |
Symmetry codes: (i) −x+1, −y, z+1/2; (ii) x, y−1, z+1. |
Acknowledgements
We gratefully acknowledge support from the National Science Foundation (CHE-1429086).
References
Bruker (2014). APEX2, SAINT, and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341. Web of Science CrossRef CAS IUCr Journals Google Scholar
Goldschmidt, G. H. & Llewellyn, F. J. (1950). Acta Cryst. 3, 294–305. CSD CrossRef CAS IUCr Journals Web of Science Google Scholar
Huang, H., Golen, J. A. & Manke, D. R. (2016). IUCrData, 1, x160007. Google Scholar
Kharbach, Y., Haoudi, A., Capet, F., Mazzah, A. & El Ammari, L. (2015). Acta Cryst. E71, o1024–o1025. Web of Science CSD CrossRef IUCr Journals Google Scholar
Kurkin, A. V., Bernovskaya, A. A., Yurovskaya, M. A. & Rybakov, V. B. (2008). Acta Cryst. E64, o1448. Web of Science CSD CrossRef IUCr Journals Google Scholar
Maamri, K., Zouihri, H., Essassi, E. M. & Ng, S. W. (2012). Acta Cryst. E68, o240. Web of Science CSD CrossRef IUCr Journals Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Sheldrick, G. M. (2015). Acta Cryst. C71, 3–8. Web of Science CrossRef IUCr Journals Google Scholar
Turbitt, J. R., Golen, J. A. & Manke, D. R. (2016). IUCrData, 1, x152434. Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.