organic compounds
A second monoclinic polymorph of 2-(diformylmethylidene)-3,3-dimethyl-2,3-dihydro-1H-indole
aDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia, and bDepartment of Molecular Medicine, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: hapipah@um.edu.my
The 13H13NO2, is a polymorph of the structure first reported by Helliwell et al. [Acta Cryst. (2006), E62, o737-o738]. It is also monoclinic (space group P21/c), but with completely different cell constants. The molecular conformations of these polymorphs differ by a 180° rotation of one formyl group. The present molecule is planar [maximum deviation 0.089 (2) Å] with the exception of the two methyl groups which lie on either side of the plane. There are strong intra- and intermolecular N—H⋯O hydrogen bonds. The latter link pairs of molecules across crystallographic centers of symmetry. Two aldehyde O atoms are brought close together [2.896 (4) Å in this arrangement but are not hydrogen bonded. In the earlier polymorph, one formyl group is rotated by 180° to yield intermolecular hydrogen bonding and an infinite polymeric chain. The other formyl group is involved in the same intramolecular hydrogen bonding as has been found here.
of the title compound, CRelated literature
For the et al. (2006). For a discussion of crystal growth conditions that can affect the occurrence of polymorphs, see: Hulliger et al. (1994). For chemistry involving 2-(diformylmethylidene)-3,3-dimethyl-2,3-dihydro-1H-indole, see: Baradarani et al. (2006).
of the other polymorph, see: HelliwellExperimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2007); cell SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2009).
Supporting information
10.1107/S1600536809038495/om2278sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809038495/om2278Isup2.hkl
A solution of trimethylindolenine, (5.57 g, 35 mmol), in anhydrous dimethylformamide (15 ml) was cooled in an ice bath. A solution of phosphoryl chloride (10 ml) in dimethylformamide (15 ml) was added dropwise with stirring over a period of 1 h at below 283 K. The cooling bath was removed and the reaction mixture was stirred at 363 K for 2 h. The resulting solution was poured onto ice water (400 ml), the pH was adjusted to 9.0 by the addition of aqueous NaOH (35%) whereupon the solid product was precipitated. It was filtered, washed with hot water, dried and recrystallized from n-hexane/ethyl acetate to give a yellow solid in 4.35 g, 58% yield. Further recrystallization, from ethanol/water (3:1 v/v), led to a mixture of lath and prismatic habits. The prism cell dimensions confirmed the form reported earlier but the laths appeared new.
C-bound hydrogen atoms were placed at calculated positions (C–H = 0.95–0.98 Å) and refined as riding with U(H) = 1.2–1.5 times Ueq(C). The N-bound hydrogen atom was located from a difference map, and freely refined to give a bond length of 0.93 (3) Å.
Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008) and publCIF (Westrip, 2009).C13H13NO2 | F(000) = 456 |
Mr = 215.24 | Dx = 1.333 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 864 reflections |
a = 6.9877 (10) Å | θ = 2.2–24.7° |
b = 18.688 (3) Å | µ = 0.09 mm−1 |
c = 8.2154 (12) Å | T = 103 K |
β = 90.291 (3)° | Lath, yellow |
V = 1072.8 (3) Å3 | 0.57 × 0.37 × 0.03 mm |
Z = 4 |
Bruker APEXII CCD diffractometer | 1865 independent reflections |
Radiation source: fine-focus sealed tube | 1123 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.072 |
ω scans | θmax = 25.1°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −5→8 |
Tmin = 0.950, Tmax = 0.997 | k = −21→22 |
4763 measured reflections | l = −9→9 |
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)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.103 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.92 | w = 1/[σ2(Fo2) + (0.0424P)2] where P = (Fo2 + 2Fc2)/3 |
1865 reflections | (Δ/σ)max < 0.001 |
151 parameters | Δρmax = 0.26 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
C13H13NO2 | V = 1072.8 (3) Å3 |
Mr = 215.24 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 6.9877 (10) Å | µ = 0.09 mm−1 |
b = 18.688 (3) Å | T = 103 K |
c = 8.2154 (12) Å | 0.57 × 0.37 × 0.03 mm |
β = 90.291 (3)° |
Bruker APEXII CCD diffractometer | 1865 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 1123 reflections with I > 2σ(I) |
Tmin = 0.950, Tmax = 0.997 | Rint = 0.072 |
4763 measured reflections |
R[F2 > 2σ(F2)] = 0.044 | 0 restraints |
wR(F2) = 0.103 | H atoms treated by a mixture of independent and constrained refinement |
S = 0.92 | Δρmax = 0.26 e Å−3 |
1865 reflections | Δρmin = −0.22 e Å−3 |
151 parameters |
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. 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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.4035 (3) | 0.49657 (9) | 0.1554 (2) | 0.0308 (5) | |
O2 | 0.4628 (3) | 0.65460 (9) | 0.6032 (2) | 0.0346 (5) | |
N1 | 0.7133 (3) | 0.57750 (10) | 0.1457 (2) | 0.0192 (5) | |
H1 | 0.637 (4) | 0.5445 (14) | 0.092 (3) | 0.054 (9)* | |
C1 | 0.6569 (3) | 0.60337 (11) | 0.2893 (3) | 0.0195 (5) | |
C2 | 0.8061 (3) | 0.65754 (12) | 0.3488 (3) | 0.0199 (6) | |
C3 | 0.9518 (3) | 0.65385 (12) | 0.2146 (3) | 0.0197 (6) | |
C4 | 1.1227 (3) | 0.68961 (12) | 0.1934 (3) | 0.0225 (6) | |
H4 | 1.1673 | 0.7228 | 0.2725 | 0.027* | |
C5 | 1.2281 (4) | 0.67584 (12) | 0.0535 (3) | 0.0253 (6) | |
H5 | 1.3459 | 0.7002 | 0.0373 | 0.030* | |
C6 | 1.1650 (4) | 0.62761 (12) | −0.0621 (3) | 0.0259 (6) | |
H6 | 1.2405 | 0.6190 | −0.1560 | 0.031* | |
C7 | 0.9931 (3) | 0.59154 (12) | −0.0434 (3) | 0.0221 (6) | |
H7 | 0.9479 | 0.5585 | −0.1226 | 0.027* | |
C8 | 0.8906 (3) | 0.60609 (11) | 0.0965 (3) | 0.0196 (5) | |
C9 | 0.4879 (3) | 0.57998 (12) | 0.3639 (3) | 0.0192 (6) | |
C10 | 0.3723 (4) | 0.52662 (12) | 0.2862 (3) | 0.0258 (6) | |
H10 | 0.2591 | 0.5128 | 0.3415 | 0.031* | |
C11 | 0.4105 (4) | 0.60552 (13) | 0.5160 (3) | 0.0257 (6) | |
H11 | 0.3018 | 0.5801 | 0.5539 | 0.031* | |
C12 | 0.7221 (4) | 0.73372 (12) | 0.3575 (3) | 0.0262 (6) | |
H12A | 0.8248 | 0.7679 | 0.3812 | 0.039* | |
H12B | 0.6261 | 0.7359 | 0.4438 | 0.039* | |
H12C | 0.6621 | 0.7458 | 0.2530 | 0.039* | |
C13 | 0.8926 (3) | 0.63454 (12) | 0.5131 (3) | 0.0241 (6) | |
H13A | 0.9436 | 0.5859 | 0.5039 | 0.036* | |
H13B | 0.7932 | 0.6357 | 0.5968 | 0.036* | |
H13C | 0.9961 | 0.6674 | 0.5433 | 0.036* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0343 (11) | 0.0320 (10) | 0.0261 (10) | −0.0086 (9) | −0.0002 (8) | −0.0040 (8) |
O2 | 0.0367 (12) | 0.0377 (11) | 0.0295 (10) | −0.0023 (9) | 0.0058 (9) | −0.0071 (9) |
N1 | 0.0143 (12) | 0.0217 (11) | 0.0215 (11) | −0.0051 (9) | 0.0010 (9) | −0.0019 (9) |
C1 | 0.0213 (15) | 0.0178 (12) | 0.0192 (12) | 0.0006 (11) | −0.0039 (11) | 0.0024 (10) |
C2 | 0.0234 (15) | 0.0187 (12) | 0.0176 (12) | −0.0011 (11) | 0.0010 (11) | −0.0001 (10) |
C3 | 0.0223 (15) | 0.0183 (12) | 0.0185 (12) | 0.0021 (11) | 0.0003 (11) | 0.0028 (10) |
C4 | 0.0205 (15) | 0.0230 (13) | 0.0239 (13) | −0.0023 (11) | −0.0024 (11) | 0.0018 (10) |
C5 | 0.0198 (15) | 0.0262 (14) | 0.0299 (14) | −0.0006 (11) | 0.0033 (12) | 0.0067 (11) |
C6 | 0.0292 (17) | 0.0253 (13) | 0.0233 (13) | 0.0041 (12) | 0.0055 (12) | 0.0039 (11) |
C7 | 0.0227 (15) | 0.0237 (13) | 0.0201 (12) | −0.0017 (11) | 0.0009 (11) | 0.0000 (10) |
C8 | 0.0208 (14) | 0.0157 (12) | 0.0223 (12) | 0.0028 (11) | 0.0000 (11) | 0.0031 (10) |
C9 | 0.0154 (14) | 0.0216 (13) | 0.0204 (12) | −0.0019 (11) | −0.0005 (11) | 0.0033 (10) |
C10 | 0.0235 (16) | 0.0267 (14) | 0.0271 (14) | −0.0004 (12) | 0.0010 (12) | 0.0077 (11) |
C11 | 0.0207 (15) | 0.0278 (14) | 0.0286 (14) | 0.0045 (12) | −0.0003 (12) | 0.0040 (12) |
C12 | 0.0313 (16) | 0.0215 (13) | 0.0259 (13) | 0.0023 (12) | 0.0020 (12) | −0.0006 (10) |
C13 | 0.0214 (15) | 0.0301 (14) | 0.0207 (13) | −0.0033 (11) | −0.0011 (11) | 0.0016 (10) |
O1—C10 | 1.233 (3) | C5—H5 | 0.9500 |
O2—C11 | 1.219 (3) | C6—C7 | 1.387 (3) |
N1—C1 | 1.336 (3) | C6—H6 | 0.9500 |
N1—C8 | 1.410 (3) | C7—C8 | 1.384 (3) |
N1—H1 | 0.93 (3) | C7—H7 | 0.9500 |
C1—C9 | 1.403 (3) | C9—C10 | 1.431 (3) |
C1—C2 | 1.531 (3) | C9—C11 | 1.445 (3) |
C2—C3 | 1.506 (3) | C10—H10 | 0.9500 |
C2—C13 | 1.538 (3) | C11—H11 | 0.9500 |
C2—C12 | 1.542 (3) | C12—H12A | 0.9800 |
C3—C4 | 1.380 (3) | C12—H12B | 0.9800 |
C3—C8 | 1.384 (3) | C12—H12C | 0.9800 |
C4—C5 | 1.392 (3) | C13—H13A | 0.9800 |
C4—H4 | 0.9500 | C13—H13B | 0.9800 |
C5—C6 | 1.380 (3) | C13—H13C | 0.9800 |
C1—N1—C8 | 112.3 (2) | C6—C7—H7 | 121.7 |
C1—N1—H1 | 119.3 (17) | C3—C8—C7 | 123.3 (2) |
C8—N1—H1 | 128.4 (17) | C3—C8—N1 | 108.2 (2) |
N1—C1—C9 | 121.7 (2) | C7—C8—N1 | 128.5 (2) |
N1—C1—C2 | 108.5 (2) | C1—C9—C10 | 119.8 (2) |
C9—C1—C2 | 129.8 (2) | C1—C9—C11 | 126.5 (2) |
C3—C2—C1 | 101.40 (18) | C10—C9—C11 | 113.8 (2) |
C3—C2—C13 | 111.46 (19) | O1—C10—C9 | 127.1 (2) |
C1—C2—C13 | 111.06 (18) | O1—C10—H10 | 116.4 |
C3—C2—C12 | 109.57 (18) | C9—C10—H10 | 116.4 |
C1—C2—C12 | 111.51 (19) | O2—C11—C9 | 130.1 (2) |
C13—C2—C12 | 111.43 (18) | O2—C11—H11 | 114.9 |
C4—C3—C8 | 119.2 (2) | C9—C11—H11 | 114.9 |
C4—C3—C2 | 131.2 (2) | C2—C12—H12A | 109.5 |
C8—C3—C2 | 109.6 (2) | C2—C12—H12B | 109.5 |
C3—C4—C5 | 118.4 (2) | H12A—C12—H12B | 109.5 |
C3—C4—H4 | 120.8 | C2—C12—H12C | 109.5 |
C5—C4—H4 | 120.8 | H12A—C12—H12C | 109.5 |
C6—C5—C4 | 121.4 (2) | H12B—C12—H12C | 109.5 |
C6—C5—H5 | 119.3 | C2—C13—H13A | 109.5 |
C4—C5—H5 | 119.3 | C2—C13—H13B | 109.5 |
C5—C6—C7 | 121.0 (2) | H13A—C13—H13B | 109.5 |
C5—C6—H6 | 119.5 | C2—C13—H13C | 109.5 |
C7—C6—H6 | 119.5 | H13A—C13—H13C | 109.5 |
C8—C7—C6 | 116.7 (2) | H13B—C13—H13C | 109.5 |
C8—C7—H7 | 121.7 |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1 | 0.93 (3) | 1.93 (3) | 2.642 (3) | 132 (2) |
N1—H1···O1i | 0.93 (3) | 2.19 (3) | 2.946 (2) | 138 (2) |
Symmetry code: (i) −x+1, −y+1, −z. |
Experimental details
Crystal data | |
Chemical formula | C13H13NO2 |
Mr | 215.24 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 103 |
a, b, c (Å) | 6.9877 (10), 18.688 (3), 8.2154 (12) |
β (°) | 90.291 (3) |
V (Å3) | 1072.8 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.57 × 0.37 × 0.03 |
Data collection | |
Diffractometer | Bruker APEXII CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.950, 0.997 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4763, 1865, 1123 |
Rint | 0.072 |
(sin θ/λ)max (Å−1) | 0.596 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.044, 0.103, 0.92 |
No. of reflections | 1865 |
No. of parameters | 151 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.26, −0.22 |
Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008) and publCIF (Westrip, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1 | 0.93 (3) | 1.93 (3) | 2.642 (3) | 132 (2) |
N1—H1···O1i | 0.93 (3) | 2.19 (3) | 2.946 (2) | 138 (2) |
Symmetry code: (i) −x+1, −y+1, −z. |
Acknowledgements
The authors thank the University of Malaya for funding this study (UMRG grant No. RG136/09HTM).
References
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