organic compounds
7-Methyl-1H-indole-2,3-dione
aDepartment of Science & Math, Massasoit Community College, 1 Massasoit Boulevard, Brockton, MA 02302, USA, and bDepartment 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, C9H7NO2, has a single molecule in the with the non-H atoms possessing a mean deviation from planarity of 0.034 Å. In the crystal, the molecules dimerize through pairs of N—H⋯O hydrogen bonds. The nine-membered rings of the isatins stack along the b axis, through parallel slipped π–π interactions [intercentroid distance = 3.8832 (4) Å, interplanar distance = 3.4038 (7) Å and slippage = 1.8690 (12) Å].
Keywords: crystal structure; isatins; hydrogen bonding; π–π interactions.
CCDC reference: 1536802
Structure description
As part of our continuing study of the intermolecular interactions of substituted isatins, we report the H-indole-2,3-dione (Fig. 1). The molecule is nearly planar, with the non-H atoms in the structure demonstrating a mean deviation from planarity of 0.034 Å. The bond lengths and angles are consistent with those observed in the reported N-substituted derivative of 7-methyl-1H-indole-2,3-dione (Mironova et al., 2015).
of 7-methyl-1In the crystal, the molecules dimerize through pairs of N1—H1⋯O1i hydrogen bonds (Table 1). This dimerization is observed in other 7-substituted isatin compounds (Garden et al., 2006; Golen & Manke, 2016a,b; Mohamed et al., 2008). The one reported exception is 7-chloroisatin, which forms a tetrameric assembly though its N—H⋯O hydrogen bonds (Sun & Cai, 2010). The nine-membered rings of the 7-methylisatin units stack along [010] with parallel slipped π–π interactions [intercentroid distance = 3.8832 (4) Å, interplanar distance = 3.4038 (7) Å and slippage = 1.8690 (12) Å]. The packing of the title compound, including hydrogen bonding, is shown in Fig. 2.
Synthesis and crystallization
A commercial sample (AK Scientific) of 7-methylisatin was recrystallized by the slow evaporation of an acetonitrile solution to yield orange plates suitable for single-crystal diffraction analysis.
Refinement
Crystal data, data collection and structure .
details are summarized in Table 2Structural data
CCDC reference: 1536802
https://doi.org/10.1107/S2414314617003789/sj4097sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314617003789/sj4097Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314617003789/sj4097Isup3.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).C9H7NO2 | F(000) = 336 |
Mr = 161.16 | Dx = 1.467 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 7.8114 (10) Å | Cell parameters from 7064 reflections |
b = 3.8832 (4) Å | θ = 2.9–25.2° |
c = 24.362 (3) Å | µ = 0.11 mm−1 |
β = 99.055 (5)° | T = 200 K |
V = 729.76 (15) Å3 | Plate, orange |
Z = 4 | 0.19 × 0.18 × 0.04 mm |
Bruker D8 Venture CMOS diffractometer | 1147 reflections with I > 2σ(I) |
φ and ω scans | Rint = 0.050 |
Absorption correction: multi-scan (SADABS; Bruker, 2014) | θmax = 25.5°, θmin = 3.4° |
Tmin = 0.701, Tmax = 0.745 | h = −9→9 |
18978 measured reflections | k = −4→4 |
1342 independent reflections | l = −29→29 |
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)] = 0.036 | w = 1/[σ2(Fo2) + (0.036P)2 + 0.3841P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.089 | (Δ/σ)max = 0.001 |
S = 1.09 | Δρmax = 0.20 e Å−3 |
1342 reflections | Δρmin = −0.17 e Å−3 |
114 parameters | Extinction correction: SHELXL2014 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
1 restraint | Extinction coefficient: 0.035 (5) |
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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.71863 (14) | −0.0390 (3) | 0.54254 (4) | 0.0339 (3) | |
O2 | 0.86187 (14) | 0.1882 (3) | 0.65601 (5) | 0.0368 (3) | |
N1 | 0.47768 (16) | 0.2518 (4) | 0.56258 (5) | 0.0245 (3) | |
H1 | 0.4086 (18) | 0.206 (5) | 0.5316 (5) | 0.029* | |
C1 | 0.64162 (19) | 0.1320 (4) | 0.57297 (6) | 0.0247 (4) | |
C2 | 0.71578 (19) | 0.2489 (4) | 0.63341 (6) | 0.0249 (4) | |
C3 | 0.57186 (19) | 0.4265 (4) | 0.65299 (6) | 0.0227 (4) | |
C4 | 0.5546 (2) | 0.5703 (4) | 0.70413 (6) | 0.0273 (4) | |
H4 | 0.6491 | 0.5730 | 0.7339 | 0.033* | |
C5 | 0.3958 (2) | 0.7094 (4) | 0.71040 (7) | 0.0303 (4) | |
H5 | 0.3804 | 0.8089 | 0.7449 | 0.036* | |
C6 | 0.2585 (2) | 0.7045 (4) | 0.66648 (7) | 0.0286 (4) | |
H6 | 0.1515 | 0.8049 | 0.6719 | 0.034* | |
C7 | 0.27078 (19) | 0.5583 (4) | 0.61465 (6) | 0.0245 (4) | |
C8 | 0.43097 (19) | 0.4204 (4) | 0.60971 (6) | 0.0217 (4) | |
C9 | 0.1214 (2) | 0.5477 (5) | 0.56768 (7) | 0.0332 (4) | |
H9A | 0.0248 | 0.6828 | 0.5776 | 0.050* | |
H9B | 0.0843 | 0.3085 | 0.5606 | 0.050* | |
H9C | 0.1575 | 0.6447 | 0.5342 | 0.050* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0267 (6) | 0.0463 (8) | 0.0293 (6) | 0.0072 (5) | 0.0062 (5) | −0.0098 (5) |
O2 | 0.0240 (6) | 0.0523 (8) | 0.0326 (6) | 0.0067 (6) | −0.0001 (5) | −0.0013 (6) |
N1 | 0.0217 (7) | 0.0307 (7) | 0.0208 (7) | 0.0019 (6) | 0.0023 (5) | −0.0027 (6) |
C1 | 0.0209 (7) | 0.0282 (8) | 0.0258 (8) | 0.0013 (7) | 0.0061 (6) | 0.0003 (7) |
C2 | 0.0233 (8) | 0.0273 (8) | 0.0243 (8) | 0.0005 (7) | 0.0045 (6) | 0.0022 (6) |
C3 | 0.0235 (8) | 0.0226 (8) | 0.0226 (8) | −0.0008 (6) | 0.0051 (6) | 0.0013 (6) |
C4 | 0.0302 (9) | 0.0282 (8) | 0.0233 (8) | −0.0022 (7) | 0.0036 (6) | −0.0007 (7) |
C5 | 0.0393 (10) | 0.0280 (9) | 0.0263 (8) | 0.0002 (7) | 0.0133 (7) | −0.0033 (7) |
C6 | 0.0290 (8) | 0.0243 (8) | 0.0356 (9) | 0.0034 (7) | 0.0146 (7) | 0.0013 (7) |
C7 | 0.0237 (8) | 0.0212 (8) | 0.0294 (8) | 0.0010 (6) | 0.0070 (6) | 0.0047 (6) |
C8 | 0.0248 (8) | 0.0198 (8) | 0.0218 (7) | −0.0007 (6) | 0.0077 (6) | 0.0025 (6) |
C9 | 0.0243 (8) | 0.0364 (10) | 0.0389 (10) | 0.0063 (7) | 0.0044 (7) | 0.0018 (8) |
O1—C1 | 1.2219 (18) | C4—C5 | 1.383 (2) |
O2—C2 | 1.2096 (18) | C5—H5 | 0.9500 |
N1—H1 | 0.875 (9) | C5—C6 | 1.391 (2) |
N1—C1 | 1.348 (2) | C6—H6 | 0.9500 |
N1—C8 | 1.4184 (19) | C6—C7 | 1.401 (2) |
C1—C2 | 1.562 (2) | C7—C8 | 1.384 (2) |
C2—C3 | 1.461 (2) | C7—C9 | 1.501 (2) |
C3—C4 | 1.391 (2) | C9—H9A | 0.9800 |
C3—C8 | 1.399 (2) | C9—H9B | 0.9800 |
C4—H4 | 0.9500 | C9—H9C | 0.9800 |
C1—N1—H1 | 122.1 (11) | C6—C5—H5 | 119.8 |
C1—N1—C8 | 111.40 (12) | C5—C6—H6 | 118.5 |
C8—N1—H1 | 126.2 (11) | C5—C6—C7 | 123.01 (15) |
O1—C1—N1 | 128.12 (14) | C7—C6—H6 | 118.5 |
O1—C1—C2 | 125.78 (13) | C6—C7—C9 | 122.86 (14) |
N1—C1—C2 | 106.09 (12) | C8—C7—C6 | 115.23 (14) |
O2—C2—C1 | 123.77 (14) | C8—C7—C9 | 121.90 (14) |
O2—C2—C3 | 131.48 (15) | C3—C8—N1 | 110.23 (13) |
C3—C2—C1 | 104.74 (12) | C7—C8—N1 | 126.90 (14) |
C4—C3—C2 | 132.06 (14) | C7—C8—C3 | 122.87 (14) |
C4—C3—C8 | 120.39 (14) | C7—C9—H9A | 109.5 |
C8—C3—C2 | 107.47 (13) | C7—C9—H9B | 109.5 |
C3—C4—H4 | 121.0 | C7—C9—H9C | 109.5 |
C5—C4—C3 | 118.09 (14) | H9A—C9—H9B | 109.5 |
C5—C4—H4 | 121.0 | H9A—C9—H9C | 109.5 |
C4—C5—H5 | 119.8 | H9B—C9—H9C | 109.5 |
C4—C5—C6 | 120.40 (15) | ||
O1—C1—C2—O2 | 2.2 (3) | C3—C4—C5—C6 | −0.1 (2) |
O1—C1—C2—C3 | −176.68 (16) | C4—C3—C8—N1 | −178.04 (14) |
O2—C2—C3—C4 | −2.8 (3) | C4—C3—C8—C7 | 1.0 (2) |
O2—C2—C3—C8 | −179.42 (17) | C4—C5—C6—C7 | 0.9 (3) |
N1—C1—C2—O2 | −179.03 (16) | C5—C6—C7—C8 | −0.7 (2) |
N1—C1—C2—C3 | 2.08 (16) | C5—C6—C7—C9 | 178.84 (15) |
C1—N1—C8—C3 | 2.46 (18) | C6—C7—C8—N1 | 178.62 (14) |
C1—N1—C8—C7 | −176.57 (15) | C6—C7—C8—C3 | −0.3 (2) |
C1—C2—C3—C4 | 175.98 (16) | C8—N1—C1—O1 | 175.98 (16) |
C1—C2—C3—C8 | −0.66 (16) | C8—N1—C1—C2 | −2.74 (17) |
C2—C3—C4—C5 | −177.07 (16) | C8—C3—C4—C5 | −0.8 (2) |
C2—C3—C8—N1 | −0.94 (17) | C9—C7—C8—N1 | −0.9 (2) |
C2—C3—C8—C7 | 178.13 (14) | C9—C7—C8—C3 | −179.79 (14) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.88 (1) | 2.03 (1) | 2.8907 (17) | 170 (2) |
Symmetry code: (i) −x+1, −y, −z+1. |
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