organic compounds
6,8-Diiodo-5,7-dimethoxy-4-methylcoumarin
aCEMDRX, Physics Department, University of Coimbra, P-3004-516 Coimbra, Portugal, and bDepartment of Chemistry, Aligarh Muslim University, Aligarh 202 002, India
*Correspondence e-mail: psidonio@pollux.fis.uc.pt
In the title compound, C12H10I2O4, the methoxy groups are twisted considerably with respect to the plane of the aromatic ring [CH3—O—C—C torsion angles = −85.9 (3) and −92.8 (3)°]. In the crystal, molecules are linked by weak C—H⋯O hydrogen bonds and O⋯I contacts [3.194 (2) Å].
Related literature
For the medicinal applications of coumarin derivatives, see: Lin et al. (2006); Massimo et al. (2003); Tyagi et al. (2003); Nawrot-Modranka et al. (2006); Sardari et al. (1999); Huang et al. (2005); Elinos-Baez et al. (2005). For the synthesis of the title compound, see: Ali & Ilyas (1986).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2003); cell SAINT (Bruker, 2003); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536810011360/bt5225sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810011360/bt5225Isup2.hkl
To a stirred solution of 5,7-dimethoxy-4-methylcoumarin (2.20 g, 10 mmol) in 15-20 ml of methanol containing 8.2 g KOH was dropwise added to a solution of I2 (2.56 g, 10 mmol) over a period of 30 min and stirred at room temperature for about 2 hours. The reaction mixture was poured into water and residual iodine was removed by washing with sodium thiosulphate. On treatment with sodium thiosulphate we obtained a precipitate which was filtered and crystallized with CHCl3—MeOH as white crystals (300 mg, m.p. 490 K).
All H atoms were located in a difference Fourier synthesis, placed in calculated positions and refined as riding on their parent atoms, using SHELXL97 (Sheldrick, 2008) defaults.
Data collection: APEX2 (Bruker, 2003); cell
SAINT (Bruker, 2003); data reduction: SAINT (Bruker, 2003); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C12H10I2O4 | F(000) = 880 |
Mr = 472.00 | Dx = 2.252 Mg m−3 |
Monoclinic, P21/c | Melting point: 490 K |
Hall symbol: -P 2ybc | Mo Kα radiation, λ = 0.71073 Å |
a = 10.8681 (2) Å | Cell parameters from 7934 reflections |
b = 9.1179 (2) Å | θ = 2.4–29.5° |
c = 17.2315 (3) Å | µ = 4.52 mm−1 |
β = 125.395 (1)° | T = 293 K |
V = 1391.95 (5) Å3 | Irregular block, pale yellow |
Z = 4 | 0.30 × 0.24 × 0.16 mm |
Bruker APEXII CCD area-detector diffractometer | 3928 independent reflections |
Radiation source: fine-focus sealed tube | 3453 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
ϕ and ω scans | θmax = 29.7°, θmin = 2.3° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | h = −14→15 |
Tmin = 0.396, Tmax = 0.485 | k = −12→12 |
27048 measured reflections | l = −24→23 |
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)] = 0.023 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.055 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0226P)2 + 1.1738P] where P = (Fo2 + 2Fc2)/3 |
3928 reflections | (Δ/σ)max = 0.001 |
166 parameters | Δρmax = 0.71 e Å−3 |
0 restraints | Δρmin = −0.96 e Å−3 |
C12H10I2O4 | V = 1391.95 (5) Å3 |
Mr = 472.00 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 10.8681 (2) Å | µ = 4.52 mm−1 |
b = 9.1179 (2) Å | T = 293 K |
c = 17.2315 (3) Å | 0.30 × 0.24 × 0.16 mm |
β = 125.395 (1)° |
Bruker APEXII CCD area-detector diffractometer | 3928 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | 3453 reflections with I > 2σ(I) |
Tmin = 0.396, Tmax = 0.485 | Rint = 0.022 |
27048 measured reflections |
R[F2 > 2σ(F2)] = 0.023 | 0 restraints |
wR(F2) = 0.055 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.71 e Å−3 |
3928 reflections | Δρmin = −0.96 e Å−3 |
166 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 | ||
I1 | 0.51053 (2) | 0.82363 (2) | 0.156895 (15) | 0.05749 (7) | |
I2 | 0.11277 (2) | 0.593603 (19) | 0.266073 (13) | 0.04546 (6) | |
O1 | 0.06827 (19) | 0.35475 (17) | 0.12276 (12) | 0.0353 (3) | |
O2 | −0.0507 (2) | 0.1432 (2) | 0.07590 (17) | 0.0548 (5) | |
O3 | 0.39384 (18) | 0.53122 (19) | 0.03873 (12) | 0.0383 (4) | |
O4 | 0.3379 (2) | 0.79647 (18) | 0.25451 (12) | 0.0434 (4) | |
C8 | 0.1966 (3) | 0.5766 (2) | 0.18397 (16) | 0.0317 (4) | |
C7 | 0.2959 (3) | 0.6823 (2) | 0.19268 (16) | 0.0337 (5) | |
C6 | 0.3586 (3) | 0.6668 (2) | 0.14197 (17) | 0.0352 (5) | |
C5 | 0.3273 (2) | 0.5453 (3) | 0.08510 (15) | 0.0318 (4) | |
C10 | 0.2315 (2) | 0.4324 (2) | 0.07795 (15) | 0.0297 (4) | |
C9 | 0.1647 (2) | 0.4549 (2) | 0.12598 (15) | 0.0294 (4) | |
C4 | 0.2056 (3) | 0.2920 (2) | 0.03026 (16) | 0.0352 (5) | |
C3 | 0.1095 (3) | 0.1972 (3) | 0.02911 (18) | 0.0395 (5) | |
H3 | 0.0905 | 0.1087 | −0.0028 | 0.047* | |
C2 | 0.0351 (3) | 0.2248 (3) | 0.07400 (18) | 0.0379 (5) | |
C13 | 0.2462 (4) | 0.9256 (3) | 0.2126 (2) | 0.0621 (8) | |
H13A | 0.2393 | 0.9513 | 0.1562 | 0.093* | |
H13B | 0.2911 | 1.0051 | 0.2573 | 0.093* | |
H13C | 0.1470 | 0.9066 | 0.1964 | 0.093* | |
C12 | 0.3139 (3) | 0.6047 (3) | −0.05204 (19) | 0.0497 (6) | |
H12A | 0.2153 | 0.5623 | −0.0936 | 0.075* | |
H12B | 0.3687 | 0.5937 | −0.0797 | 0.075* | |
H12C | 0.3044 | 0.7070 | −0.0433 | 0.075* | |
C11 | 0.2873 (4) | 0.2436 (3) | −0.0117 (2) | 0.0582 (8) | |
H11A | 0.2607 | 0.1440 | −0.0331 | 0.087* | |
H11B | 0.3942 | 0.2502 | 0.0357 | 0.087* | |
H11C | 0.2592 | 0.3057 | −0.0646 | 0.087* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.05881 (12) | 0.05243 (11) | 0.06135 (13) | −0.02587 (9) | 0.03486 (10) | −0.01030 (8) |
I2 | 0.05746 (11) | 0.04523 (10) | 0.04782 (10) | −0.00537 (7) | 0.03859 (9) | −0.01056 (7) |
O1 | 0.0400 (9) | 0.0303 (7) | 0.0438 (9) | −0.0055 (6) | 0.0290 (8) | −0.0069 (7) |
O2 | 0.0650 (13) | 0.0391 (9) | 0.0823 (15) | −0.0165 (9) | 0.0552 (12) | −0.0145 (10) |
O3 | 0.0370 (8) | 0.0458 (9) | 0.0384 (9) | 0.0023 (7) | 0.0255 (8) | 0.0035 (7) |
O4 | 0.0572 (11) | 0.0325 (8) | 0.0355 (9) | −0.0062 (8) | 0.0239 (8) | −0.0092 (7) |
C8 | 0.0355 (11) | 0.0304 (10) | 0.0307 (10) | 0.0031 (8) | 0.0200 (9) | −0.0015 (8) |
C7 | 0.0380 (12) | 0.0277 (10) | 0.0286 (10) | −0.0006 (8) | 0.0154 (9) | −0.0023 (8) |
C6 | 0.0355 (11) | 0.0325 (11) | 0.0330 (11) | −0.0057 (9) | 0.0172 (10) | 0.0007 (9) |
C5 | 0.0299 (10) | 0.0357 (11) | 0.0291 (10) | 0.0019 (8) | 0.0167 (9) | 0.0032 (8) |
C10 | 0.0307 (10) | 0.0294 (10) | 0.0271 (10) | 0.0008 (8) | 0.0157 (9) | −0.0008 (8) |
C9 | 0.0293 (10) | 0.0280 (9) | 0.0296 (10) | 0.0003 (8) | 0.0162 (9) | −0.0005 (8) |
C4 | 0.0400 (12) | 0.0334 (11) | 0.0338 (11) | 0.0017 (9) | 0.0224 (10) | −0.0036 (9) |
C3 | 0.0477 (14) | 0.0299 (11) | 0.0453 (13) | −0.0041 (10) | 0.0294 (12) | −0.0077 (9) |
C2 | 0.0409 (12) | 0.0290 (10) | 0.0453 (13) | −0.0031 (9) | 0.0257 (11) | −0.0049 (9) |
C13 | 0.093 (2) | 0.0340 (13) | 0.0625 (19) | 0.0072 (15) | 0.0471 (19) | −0.0025 (12) |
C12 | 0.0480 (15) | 0.0696 (18) | 0.0379 (13) | 0.0039 (13) | 0.0285 (12) | 0.0077 (12) |
C11 | 0.078 (2) | 0.0493 (16) | 0.077 (2) | −0.0089 (15) | 0.0618 (19) | −0.0206 (15) |
I1—C6 | 2.084 (2) | C10—C4 | 1.458 (3) |
I2—C8 | 2.085 (2) | C4—C3 | 1.347 (3) |
O1—C9 | 1.367 (3) | C4—C11 | 1.500 (3) |
O1—C2 | 1.375 (3) | C3—C2 | 1.428 (3) |
O2—C2 | 1.208 (3) | C3—H3 | 0.9300 |
O3—C5 | 1.359 (3) | C13—H13A | 0.9600 |
O3—C12 | 1.441 (3) | C13—H13B | 0.9600 |
O4—C7 | 1.365 (3) | C13—H13C | 0.9600 |
O4—C13 | 1.438 (3) | C12—H12A | 0.9600 |
C8—C7 | 1.389 (3) | C12—H12B | 0.9600 |
C8—C9 | 1.396 (3) | C12—H12C | 0.9600 |
C7—C6 | 1.392 (3) | C11—H11A | 0.9600 |
C6—C5 | 1.385 (3) | C11—H11B | 0.9600 |
C5—C10 | 1.418 (3) | C11—H11C | 0.9600 |
C10—C9 | 1.397 (3) | ||
C9—O1—C2 | 121.60 (18) | C4—C3—C2 | 123.8 (2) |
C5—O3—C12 | 113.74 (18) | C4—C3—H3 | 118.1 |
C7—O4—C13 | 114.3 (2) | C2—C3—H3 | 118.1 |
C7—C8—C9 | 118.9 (2) | O2—C2—O1 | 116.6 (2) |
C7—C8—I2 | 119.53 (16) | O2—C2—C3 | 126.5 (2) |
C9—C8—I2 | 121.34 (16) | O1—C2—C3 | 116.9 (2) |
O4—C7—C8 | 120.0 (2) | O4—C13—H13A | 109.5 |
O4—C7—C6 | 120.2 (2) | O4—C13—H13B | 109.5 |
C8—C7—C6 | 119.6 (2) | H13A—C13—H13B | 109.5 |
C5—C6—C7 | 121.1 (2) | O4—C13—H13C | 109.5 |
C5—C6—I1 | 119.26 (17) | H13A—C13—H13C | 109.5 |
C7—C6—I1 | 119.58 (16) | H13B—C13—H13C | 109.5 |
O3—C5—C6 | 119.7 (2) | O3—C12—H12A | 109.5 |
O3—C5—C10 | 119.6 (2) | O3—C12—H12B | 109.5 |
C6—C5—C10 | 120.6 (2) | H12A—C12—H12B | 109.5 |
C9—C10—C5 | 116.74 (19) | O3—C12—H12C | 109.5 |
C9—C10—C4 | 117.8 (2) | H12A—C12—H12C | 109.5 |
C5—C10—C4 | 125.4 (2) | H12B—C12—H12C | 109.5 |
O1—C9—C10 | 121.85 (19) | C4—C11—H11A | 109.5 |
O1—C9—C8 | 115.25 (19) | C4—C11—H11B | 109.5 |
C10—C9—C8 | 122.8 (2) | H11A—C11—H11B | 109.5 |
C3—C4—C10 | 117.8 (2) | C4—C11—H11C | 109.5 |
C3—C4—C11 | 118.3 (2) | H11A—C11—H11C | 109.5 |
C10—C4—C11 | 123.7 (2) | H11B—C11—H11C | 109.5 |
C13—O4—C7—C8 | −92.8 (3) | C2—O1—C9—C10 | 1.7 (3) |
C13—O4—C7—C6 | 90.7 (3) | C2—O1—C9—C8 | −175.3 (2) |
C9—C8—C7—O4 | −175.0 (2) | C5—C10—C9—O1 | 178.85 (19) |
I2—C8—C7—O4 | −0.1 (3) | C4—C10—C9—O1 | −5.2 (3) |
C9—C8—C7—C6 | 1.5 (3) | C5—C10—C9—C8 | −4.3 (3) |
I2—C8—C7—C6 | 176.40 (17) | C4—C10—C9—C8 | 171.7 (2) |
O4—C7—C6—C5 | 174.5 (2) | C7—C8—C9—O1 | 178.8 (2) |
C8—C7—C6—C5 | −2.0 (3) | I2—C8—C9—O1 | 4.0 (3) |
O4—C7—C6—I1 | −2.4 (3) | C7—C8—C9—C10 | 1.7 (3) |
C8—C7—C6—I1 | −178.96 (17) | I2—C8—C9—C10 | −173.05 (16) |
C12—O3—C5—C6 | −85.9 (3) | C9—C10—C4—C3 | 5.1 (3) |
C12—O3—C5—C10 | 96.7 (3) | C5—C10—C4—C3 | −179.3 (2) |
C7—C6—C5—O3 | −178.0 (2) | C9—C10—C4—C11 | −170.8 (3) |
I1—C6—C5—O3 | −1.1 (3) | C5—C10—C4—C11 | 4.8 (4) |
C7—C6—C5—C10 | −0.7 (3) | C10—C4—C3—C2 | −1.8 (4) |
I1—C6—C5—C10 | 176.25 (16) | C11—C4—C3—C2 | 174.3 (3) |
O3—C5—C10—C9 | −178.92 (19) | C9—O1—C2—O2 | 179.6 (2) |
C6—C5—C10—C9 | 3.7 (3) | C9—O1—C2—C3 | 1.7 (3) |
O3—C5—C10—C4 | 5.4 (3) | C4—C3—C2—O2 | −179.2 (3) |
C6—C5—C10—C4 | −171.9 (2) | C4—C3—C2—O1 | −1.7 (4) |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···O2i | 0.93 | 2.53 | 3.460 (3) | 175 |
Symmetry code: (i) −x, −y, −z. |
Experimental details
Crystal data | |
Chemical formula | C12H10I2O4 |
Mr | 472.00 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 293 |
a, b, c (Å) | 10.8681 (2), 9.1179 (2), 17.2315 (3) |
β (°) | 125.395 (1) |
V (Å3) | 1391.95 (5) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.52 |
Crystal size (mm) | 0.30 × 0.24 × 0.16 |
Data collection | |
Diffractometer | Bruker APEXII CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2003) |
Tmin, Tmax | 0.396, 0.485 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 27048, 3928, 3453 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.697 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.023, 0.055, 1.06 |
No. of reflections | 3928 |
No. of parameters | 166 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.71, −0.96 |
Computer programs: APEX2 (Bruker, 2003), SAINT (Bruker, 2003), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3···O2i | 0.93 | 2.53 | 3.460 (3) | 175.1 |
Symmetry code: (i) −x, −y, −z. |
Acknowledgements
This work was supported by the Fundação para a Ciência e a Tecnologia (FCT) under scholarship SFRH/BD/38387/2008.
References
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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.
Coumarin is the simplest member of the group of oxygen heterocyclics called benzo-2-pyrone. Coumarins are an important class of compounds due to their presence in natural products as well as their medicinal applications such as anti-inflammatory (Lin et al., 2006), anti-viral (Massimo et al., 2003), antioxidant (Tyagi et al., 2003), antibacterial (Nawrot-Modranka et al., 2006), antifungal (Sardari et al., 1999), anti-HIV (Huang et al., 2005) and as anti-carcinogenic (Elinos-Baez et al., 2005). Besides the wide spectrum of biological applications of coumarin and its derivatives, the chemical literature also embodies their applications as cosmetics, optical brightening agents, and laser dyes. A recent report has revealed the anion sensing ability of some coumarin derivatives. Among various coumarin derivatives, recent pharmacological evaluation of iodocoumarins as cannabinoid receptor antagonists and inverse agonists has been done. Iodocoumarins such as 8-iodo-7-hydroxycoumarin exhibited moderate activity and 8-iodo-5,7-dihydroxycoumarin displayed good antimicrobial properties with MIC values <100 µg/ml. Also, iodocoumarins had been successfully used for the optimization of reaction conditions and kinetic studies in high throughput format. Because of the biological and pharmaceutical importance of iodocoumarins, several protocols for the synthesis have been reported.
In the light of the mentioned above we planned to synthesize iodocoumarins by reaction of 5,7-dimethoxy-4-methylcoumarin with iodine in basic media (Ali & Ilyas, 1986).
In the molecule of the title compound (Fig. 1), the best plane through the aromatic ring shows an r.m.s. deviation of 0.0154 Å; the O1—C2—C3—C4—C10—C9 ring shows a slightly larger deviation from planarity, with an r.m.s. deviation of 0.0189 Å. The angle between these two planes is 4.96 (11)°.
The C2 atom of the carbonyl group has a distorted trigonal geometry with O2—C2—O1 [116.6 (2)°] and O2—C2—C3 [126.5 (2)°] deviating significantly from the ideal sp2 value of 120°.
The methoxy groups are considerably twisted with respect to the plane of the aromatic ring as indicated by the torsion angles C12—O3—C5—C6 [-85.9 (3)°] and C13—O4—C7—C6 [90.7 (3)°]. The iodine atoms are almost in the plane of the benzene ring and the methyl group is slightly out of the pyrone ring plane.
The molecules are linked across an inversion centre by one weak hydrogen bond of the C—H···O type (Fig. 2, Table 2).