Abstract
The crystal structure of the title compound, C11H9NO4, consists of infinite one-dimensional polymeric chains due to intermolecular O—H⋯O hydrogen bonds between the carboxylate and carbonyl groups. The phthalimide ring system and the C—COO group are planar, with r.m.s. deviations of 0.0253 and 0.0067 Å, respectively, from their mean square planes and the dihedral angle between them is 66.41 (7)°. The molecules are stabilized by C=O⋯π interactions and weak intramolecular C—H⋯O hydrogen bonds.
Related literature
For the medicinal properties of isocoumarin, see: Matsuda et al. (1999 ▶). For related crystal structures, see: Li & Liang (2006 ▶); Raza et al. (2009 ▶); Wheeler et al. (2004 ▶). For the graph-set analysis of hydrogen-bond patterns in crystal structures, see: Bernstein et al. (1995 ▶).
Experimental
Crystal data
C11H9NO4
M r = 219.19
Monoclinic,
a = 9.3056 (8) Å
b = 5.9768 (4) Å
c = 9.7583 (8) Å
β = 110.988 (3)°
V = 506.73 (7) Å3
Z = 2
Mo Kα radiation
μ = 0.11 mm−1
T = 296 K
0.30 × 0.25 × 0.23 mm
Data collection
Bruker Kappa APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2005 ▶) T min = 0.968, T max = 0.974
5705 measured reflections
1381 independent reflections
1302 reflections with I > 2σ(I)
R int = 0.023
Refinement
R[F 2 > 2σ(F 2)] = 0.030
wR(F 2) = 0.082
S = 1.06
1381 reflections
153 parameters
1 restraint
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.16 e Å−3
Δρmin = −0.13 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: 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: ORTEP-3 for Windows (Farrugia, 1997 ▶) and PLATON (Spek, 2009 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶) and PLATON.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809040434/si2209sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809040434/si2209Isup2.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 |
|---|---|---|---|---|
| O3—H3A⋯O1i | 0.80 (4) | 1.96 (4) | 2.750 (2) | 172 (4) |
| C9—H9⋯O2 | 0.96 (3) | 2.48 (2) | 2.899 (2) | 106.6 (17) |
| C8—O2⋯Cg1ii | 1.20 (1) | 3.09 (1) | 4.0543 (17) | 138 (1) |
Symmetry codes: (i)
; (ii)
. Cg1 is the centroid of 5-membered heterocyclic ring.
Acknowledgments
The authors acknowledge the Higher Education Commission, Islamabad, Pakistan, and Bana International, Karachi, Pakistan, for funding the purchase of the diffractometer and for technical support, respectively.
supplementary crystallographic information
Comment
Isocoumarin are important components among natural products that exhibit a broad range of biological activities including anti-microbial, anti-allergic and immunomodulatory (Matsuda et al., 1999). Isocoumarins are also useful intermediates in synthesis of many important compounds e.g., isoquinoline alkaloids. The titled compound (I, Fig. 1), is an intermediate towards the synthesis of isocoumarins. The title compound has also been prepared for complexation with various metals.
We have recently reported the crystal structure of (II) (2R)-2-(1,3-Dioxoisoindolin-2-yl)-4-(methylsulfanyl)butanoic acid (Raza et al., 2009) which contain the same isoindoline. The crystal structures of (III) DL-2-(1,3-Dioxoisoindolin-2-yl)propanoic acid (Wheeler et al., 2004), (IV) (S)-2-(1,3-Dioxoisoindolin-2-yl)propanoic acid (Li & Liang, 2006) have also been reported which are the racemate of (I).
In (I) the phthalimide ring system A (C1—C8/N1/O1/O2) and the group B (C9/C10/O3/O4) are planar with r.m.s. deviations of 0.0253 and 0.0067 Å respectively, from their mean square planes. The dihedral angle between A/B is 66.41 (7)°, whereas it is 86.7 (3)° as observed in (IV). The title compound is stabilized in the form of infinite one dimensional polymeric chains due to intermolecular H-bondings (Table 1, Fig. 2). There exist a weak intramolecular H-bondings forming S(5) ring motifs (Fig. 1) (Bernstein et al., 1995). The C==O···Cg1 [Cg1 is the centroid of five membered ring (C1/C2/C7/C8/N1)] interaction (Table 1), may also be responsible for stabilizing of the molecules.
Experimental
The (S)-alanine (1.96 g, 22 mmol) and phthallic anhydride (3.6 g, 24.3 mmol) were added to a flask with constant stirring. The temperature of oil bath was kept at 433 K. Three hours later the flask was removed from oil bath, brought to room temperature and the crystals of phthallic anhydride on the walls of the flask were removed manually. The solid crude product was purified by crystallization from ethanol:water (8:2) that yielded (70%) colorless prisms of the title compound (I).
Refinement
In the absence of significant anomalous dispersion effects, Friedel pairs were averaged using MERG 3.
The coordinates of H3A and H9 were refined. The H-atoms were positioned geometrically with C—H = 0.93 and 0.96 Å for aromatic and methyl H atoms respectively and constrained to ride on their parent atoms, with Uiso(H) = xUeq(C, O), where x = 1.5 for methyl and 1.2 for all other H atoms.
Figures
Fig. 1.
View of (I) with the atom numbering scheme. The thermal ellipsoids are drawn at the 50% probability level. H-atoms are shown by small circles of arbitrary radii. The dotted line represent the intramolecular H-bonding.
Fig. 2.
The partial packing (PLATON; Spek, 2009) which shows that molecules form infinite one dimensional polymeric chains.
Crystal data
| C11H9NO4 | F(000) = 228 |
| Mr = 219.19 | Dx = 1.437 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 2319 reflections |
| a = 9.3056 (8) Å | θ = 2.2–28.3° |
| b = 5.9768 (4) Å | µ = 0.11 mm−1 |
| c = 9.7583 (8) Å | T = 296 K |
| β = 110.988 (3)° | Prism, colorless |
| V = 506.73 (7) Å3 | 0.30 × 0.25 × 0.23 mm |
| Z = 2 |
Data collection
| Bruker Kappa APEXII CCD diffractometer | 1381 independent reflections |
| Radiation source: fine-focus sealed tube | 1302 reflections with I > 2σ(I) |
| graphite | Rint = 0.023 |
| Detector resolution: 7.40 pixels mm-1 | θmax = 28.3°, θmin = 2.2° |
| ω scans | h = −12→12 |
| Absorption correction: multi-scan (SADABS; Bruker, 2005) | k = −7→7 |
| Tmin = 0.968, Tmax = 0.974 | l = −12→13 |
| 5705 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.030 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.082 | w = 1/[σ2(Fo2) + (0.0443P)2 + 0.0584P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.06 | (Δ/σ)max < 0.001 |
| 1381 reflections | Δρmax = 0.16 e Å−3 |
| 153 parameters | Δρmin = −0.13 e Å−3 |
| 1 restraint | Extinction correction: SHELXL97 (Sheldrick, 2008) |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.132 (13) |
Special details
| Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
| 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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| O1 | 0.34281 (15) | 1.0490 (3) | 0.31137 (15) | 0.0551 (4) | |
| O2 | −0.00322 (14) | 0.5031 (3) | 0.09136 (15) | 0.0520 (4) | |
| O3 | 0.41497 (15) | 0.5761 (3) | 0.42520 (15) | 0.0550 (5) | |
| O4 | 0.57532 (16) | 0.5164 (5) | 0.30695 (19) | 0.0817 (7) | |
| N1 | 0.19830 (14) | 0.7462 (3) | 0.19714 (14) | 0.0358 (4) | |
| C1 | 0.22202 (19) | 0.9473 (3) | 0.27082 (17) | 0.0382 (4) | |
| C2 | 0.07493 (19) | 1.0033 (3) | 0.28948 (17) | 0.0402 (5) | |
| C3 | 0.0385 (3) | 1.1806 (4) | 0.3606 (2) | 0.0562 (6) | |
| C4 | −0.1092 (3) | 1.1832 (5) | 0.3656 (2) | 0.0690 (8) | |
| C5 | −0.2125 (3) | 1.0146 (6) | 0.3031 (2) | 0.0684 (9) | |
| C6 | −0.1755 (2) | 0.8353 (5) | 0.2313 (2) | 0.0539 (6) | |
| C7 | −0.02955 (19) | 0.8354 (3) | 0.22485 (16) | 0.0392 (4) | |
| C8 | 0.04667 (17) | 0.6700 (3) | 0.16030 (16) | 0.0361 (4) | |
| C9 | 0.31769 (19) | 0.6226 (4) | 0.1658 (2) | 0.0432 (5) | |
| C10 | 0.45173 (19) | 0.5679 (4) | 0.3068 (2) | 0.0470 (5) | |
| C11 | 0.3710 (3) | 0.7438 (6) | 0.0556 (2) | 0.0642 (8) | |
| H3 | 0.10903 | 1.29359 | 0.40332 | 0.0674* | |
| H3A | 0.490 (4) | 0.564 (6) | 0.497 (4) | 0.0660* | |
| H4 | −0.13859 | 1.30102 | 0.41199 | 0.0828* | |
| H5 | −0.30990 | 1.02072 | 0.30905 | 0.0820* | |
| H6 | −0.24537 | 0.72111 | 0.18964 | 0.0647* | |
| H9 | 0.273 (2) | 0.482 (5) | 0.125 (2) | 0.0518* | |
| H11A | 0.28411 | 0.77266 | −0.03225 | 0.0962* | |
| H11B | 0.44407 | 0.65239 | 0.03244 | 0.0962* | |
| H11C | 0.41850 | 0.88289 | 0.09692 | 0.0962* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0464 (7) | 0.0507 (8) | 0.0545 (7) | −0.0167 (7) | 0.0015 (5) | −0.0070 (7) |
| O2 | 0.0474 (7) | 0.0484 (8) | 0.0563 (7) | −0.0153 (6) | 0.0139 (6) | −0.0153 (7) |
| O3 | 0.0409 (6) | 0.0693 (10) | 0.0459 (7) | 0.0152 (7) | 0.0046 (5) | 0.0073 (7) |
| O4 | 0.0412 (7) | 0.1193 (17) | 0.0869 (11) | 0.0252 (10) | 0.0257 (8) | 0.0306 (13) |
| N1 | 0.0288 (6) | 0.0363 (7) | 0.0363 (6) | 0.0000 (5) | 0.0042 (5) | −0.0024 (6) |
| C1 | 0.0385 (8) | 0.0368 (8) | 0.0310 (7) | −0.0025 (7) | 0.0024 (6) | −0.0004 (6) |
| C2 | 0.0470 (9) | 0.0382 (9) | 0.0311 (7) | 0.0044 (7) | 0.0088 (6) | 0.0021 (7) |
| C3 | 0.0773 (13) | 0.0452 (11) | 0.0407 (8) | 0.0125 (10) | 0.0147 (9) | −0.0034 (8) |
| C4 | 0.0893 (16) | 0.0758 (17) | 0.0461 (10) | 0.0356 (15) | 0.0293 (10) | 0.0019 (11) |
| C5 | 0.0612 (12) | 0.098 (2) | 0.0532 (11) | 0.0276 (14) | 0.0292 (10) | 0.0102 (13) |
| C6 | 0.0444 (9) | 0.0727 (14) | 0.0478 (9) | 0.0048 (10) | 0.0203 (8) | 0.0056 (10) |
| C7 | 0.0382 (7) | 0.0451 (9) | 0.0314 (7) | 0.0023 (7) | 0.0089 (6) | 0.0036 (7) |
| C8 | 0.0327 (7) | 0.0384 (8) | 0.0325 (7) | −0.0032 (7) | 0.0060 (5) | 0.0005 (6) |
| C9 | 0.0346 (8) | 0.0473 (10) | 0.0444 (8) | 0.0009 (8) | 0.0102 (6) | −0.0067 (8) |
| C10 | 0.0338 (7) | 0.0475 (10) | 0.0566 (10) | 0.0031 (8) | 0.0126 (7) | 0.0069 (9) |
| C11 | 0.0556 (11) | 0.0928 (18) | 0.0468 (10) | 0.0056 (13) | 0.0217 (8) | 0.0027 (12) |
Geometric parameters (Å, °)
| O1—C1 | 1.213 (2) | C5—C6 | 1.390 (4) |
| O2—C8 | 1.200 (2) | C6—C7 | 1.382 (3) |
| O3—C10 | 1.318 (2) | C7—C8 | 1.482 (2) |
| O4—C10 | 1.190 (3) | C9—C10 | 1.525 (3) |
| O3—H3A | 0.80 (4) | C9—C11 | 1.520 (3) |
| N1—C8 | 1.402 (2) | C3—H3 | 0.9300 |
| N1—C9 | 1.455 (3) | C4—H4 | 0.9300 |
| N1—C1 | 1.377 (2) | C5—H5 | 0.9300 |
| C1—C2 | 1.482 (3) | C6—H6 | 0.9300 |
| C2—C3 | 1.374 (3) | C9—H9 | 0.96 (3) |
| C2—C7 | 1.382 (2) | C11—H11A | 0.9600 |
| C3—C4 | 1.393 (4) | C11—H11B | 0.9600 |
| C4—C5 | 1.375 (4) | C11—H11C | 0.9600 |
| O1···O3 | 3.023 (2) | C5···C11viii | 3.551 (3) |
| O1···C10 | 3.055 (3) | C6···O4ix | 3.283 (3) |
| O1···C10i | 3.268 (3) | C7···O2viii | 3.361 (2) |
| O1···C11 | 3.177 (3) | C8···O2viii | 3.074 (2) |
| O1···O3ii | 2.750 (2) | C8···C3iv | 3.534 (3) |
| O2···C7iii | 3.361 (2) | C10···O1 | 3.055 (3) |
| O2···N1iii | 3.149 (2) | C10···O1iv | 3.268 (3) |
| O2···C3iv | 3.168 (3) | C11···C5iii | 3.551 (3) |
| O2···C8iii | 3.074 (2) | C11···O1 | 3.177 (3) |
| O2···C1iii | 3.405 (2) | C1···H3Aii | 2.91 (4) |
| O3···N1 | 2.615 (2) | C1···H11C | 2.9300 |
| O3···O1 | 3.023 (2) | C2···H4x | 3.0100 |
| O3···C1 | 2.912 (2) | C3···H4x | 3.0800 |
| O3···O1v | 2.750 (2) | C5···H3x | 2.9800 |
| O4···C6vi | 3.283 (3) | C5···H11Aviii | 2.9200 |
| O1···H3Aii | 1.96 (4) | H3···C5xi | 2.9800 |
| O1···H11C | 2.6300 | H3A···O1v | 1.96 (4) |
| O2···H11Aiii | 2.8300 | H3A···C1v | 2.91 (4) |
| O2···H9 | 2.48 (2) | H4···O4xii | 2.8000 |
| O4···H4vii | 2.8000 | H4···C2xi | 3.0100 |
| O4···H6vi | 2.6400 | H4···C3xi | 3.0800 |
| O4···H11B | 2.6400 | H6···O4ix | 2.6400 |
| N1···O3 | 2.615 (2) | H9···O2 | 2.48 (2) |
| N1···O2viii | 3.149 (2) | H11A···O2viii | 2.8300 |
| C1···O3 | 2.912 (2) | H11A···C5iii | 2.9200 |
| C1···O2viii | 3.405 (2) | H11B···O4 | 2.6400 |
| C3···C8i | 3.534 (3) | H11C···O1 | 2.6300 |
| C3···O2i | 3.168 (3) | H11C···C1 | 2.9300 |
| C10—O3—H3A | 110 (3) | N1—C9—C10 | 111.01 (15) |
| C1—N1—C9 | 124.14 (15) | O3—C10—C9 | 113.43 (16) |
| C8—N1—C9 | 123.75 (16) | O4—C10—C9 | 122.29 (18) |
| C1—N1—C8 | 112.08 (15) | O3—C10—O4 | 124.24 (19) |
| O1—C1—C2 | 129.45 (17) | C2—C3—H3 | 122.00 |
| N1—C1—C2 | 106.19 (15) | C4—C3—H3 | 122.00 |
| O1—C1—N1 | 124.35 (17) | C3—C4—H4 | 119.00 |
| C1—C2—C3 | 129.93 (19) | C5—C4—H4 | 119.00 |
| C3—C2—C7 | 122.00 (19) | C4—C5—H5 | 119.00 |
| C1—C2—C7 | 108.03 (15) | C6—C5—H5 | 119.00 |
| C2—C3—C4 | 116.8 (2) | C5—C6—H6 | 122.00 |
| C3—C4—C5 | 121.2 (3) | C7—C6—H6 | 122.00 |
| C4—C5—C6 | 121.9 (3) | N1—C9—H9 | 106.4 (13) |
| C5—C6—C7 | 116.6 (2) | C10—C9—H9 | 106.2 (13) |
| C2—C7—C6 | 121.44 (18) | C11—C9—H9 | 109.1 (12) |
| C2—C7—C8 | 108.22 (16) | C9—C11—H11A | 109.00 |
| C6—C7—C8 | 130.30 (18) | C9—C11—H11B | 109.00 |
| O2—C8—N1 | 124.46 (16) | C9—C11—H11C | 109.00 |
| O2—C8—C7 | 130.15 (16) | H11A—C11—H11B | 109.00 |
| N1—C8—C7 | 105.39 (14) | H11A—C11—H11C | 109.00 |
| N1—C9—C11 | 112.0 (2) | H11B—C11—H11C | 109.00 |
| C10—C9—C11 | 111.83 (17) | ||
| C8—N1—C1—O1 | −178.37 (16) | C1—C2—C7—C6 | 176.60 (16) |
| C8—N1—C1—C2 | 2.54 (18) | C1—C2—C7—C8 | −1.21 (18) |
| C9—N1—C1—O1 | 3.8 (3) | C3—C2—C7—C6 | −1.4 (3) |
| C9—N1—C1—C2 | −175.31 (15) | C3—C2—C7—C8 | −179.17 (16) |
| C1—N1—C8—O2 | 177.22 (16) | C2—C3—C4—C5 | 0.5 (3) |
| C1—N1—C8—C7 | −3.24 (18) | C3—C4—C5—C6 | −0.5 (4) |
| C9—N1—C8—O2 | −4.9 (3) | C4—C5—C6—C7 | −0.4 (3) |
| C9—N1—C8—C7 | 174.62 (15) | C5—C6—C7—C2 | 1.3 (3) |
| C1—N1—C9—C10 | 57.8 (2) | C5—C6—C7—C8 | 178.61 (18) |
| C1—N1—C9—C11 | −67.9 (2) | C2—C7—C8—O2 | −177.83 (18) |
| C8—N1—C9—C10 | −119.78 (18) | C2—C7—C8—N1 | 2.66 (17) |
| C8—N1—C9—C11 | 114.5 (2) | C6—C7—C8—O2 | 4.6 (3) |
| O1—C1—C2—C3 | −2.0 (3) | C6—C7—C8—N1 | −174.88 (18) |
| O1—C1—C2—C7 | −179.76 (18) | N1—C9—C10—O3 | 20.4 (3) |
| N1—C1—C2—C3 | 177.02 (18) | N1—C9—C10—O4 | −161.9 (3) |
| N1—C1—C2—C7 | −0.73 (18) | C11—C9—C10—O3 | 146.2 (2) |
| C1—C2—C3—C4 | −177.09 (18) | C11—C9—C10—O4 | −36.0 (4) |
| C7—C2—C3—C4 | 0.4 (3) |
Symmetry codes: (i) x, y+1, z; (ii) −x+1, y+1/2, −z+1; (iii) −x, y−1/2, −z; (iv) x, y−1, z; (v) −x+1, y−1/2, −z+1; (vi) x+1, y, z; (vii) x+1, y−1, z; (viii) −x, y+1/2, −z; (ix) x−1, y, z; (x) −x, y−1/2, −z+1; (xi) −x, y+1/2, −z+1; (xii) x−1, y+1, z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O3—H3A···O1v | 0.80 (4) | 1.96 (4) | 2.750 (2) | 172 (4) |
| C9—H9···O2 | 0.96 (3) | 2.48 (2) | 2.899 (2) | 106.6 (17) |
| C8—O2···Cg1iii | 1.200 (2) | 3.0874 (16) | 4.0543 (17) | 138.28 (12) |
Symmetry codes: (v) −x+1, y−1/2, −z+1; (iii) −x, y−1/2, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2209).
References
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- Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
- Farrugia, L. J. (1999). J. Appl. Cryst.32, 837–838.
- Li, J. & Liang, Z.-P. (2006). Acta Cryst. E62, o4915–o4916.
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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/S1600536809040434/si2209sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809040434/si2209Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


