| Literature DB >> 28775879 |
Igor Elkin1, Thierry Maris2, Patrice Hildgen1.
Abstract
The number of known asymmetrically substituted hemilactides, important precursors for obtaining regular derivatives of polylactide polymers, is still limited and structural characterization of most of them is incomplete. In the title racemic 1,4-dioxane-2,5-dione derivative, C9H10O5, the hemilactide heterocycle exhibits a twist-boat conformation. The bulkier propynyloxymethyl group is in an axial position with a gauche conformation for the CH2-O-CH2-C segment. In the crystal, mol-ecules are linked by pairs of C-H⋯O hydrogen bonds, forming inversion dimers. The dimers are linked by further C-H⋯O contacts, forming a three-dimensional structure.Entities:
Keywords: 3-methyl-6-propynyloxymethyl-1,4-dioxane-2,5-dione; crystal structure; lactide; synthesis
Year: 2017 PMID: 28775879 PMCID: PMC5499287 DOI: 10.1107/S2056989017008581
Source DB: PubMed Journal: Acta Crystallogr E Crystallogr Commun
Figure 1The atom-numbering diagram of the molecule of 1. C and O atoms are shown as displacement ellipsoids at the 50% probability level and H atoms are shown as spheres of arbitrary radius.
Figure 2A view along the b axis of the crystal packing of 1. Weak C—H⋯O contacts involving the acetylenyl H and ketone O atoms are shown as dotted lines.
Hydrogen-bond geometry (Å, °)
|
|
| H⋯ |
|
|
|---|---|---|---|---|
| C3—H3⋯O4i | 0.92 (2) | 2.60 (2) | 3.247 (3) | 127.8 (16) |
| C3—H3⋯O5 | 0.92 (2) | 2.49 (2) | 3.033 (2) | 118.1 (16) |
| C6—H6 | 0.99 (3) | 2.47 (2) | 3.369 (3) | 151.0 (19) |
| C7—H7 | 0.98 (2) | 2.66 (2) | 3.627 (3) | 169.1 (18) |
| C9—H9⋯O4iv | 0.88 (3) | 2.58 (3) | 3.412 (3) | 156 (2) |
Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .
Figure 3Scheme of the chemical synthesis of the title compound 3-methyl-6-[(propynyloxy)methyl]-1,4-dioxane-2,5-dione (1).
Experimental details
| Crystal data | |
| Chemical formula | C9H10O5 |
|
| 198.17 |
| Crystal system, space group | Monoclinic, |
| Temperature (K) | 100 |
|
| 6.9774 (5), 6.8273 (5), 19.4895 (14) |
| β (°) | 95.804 (3) |
|
| 923.66 (12) |
|
| 4 |
| Radiation type | Ga |
| μ (mm−1) | 0.65 |
| Crystal size (mm) | 0.11 × 0.08 × 0.08 |
| Data collection | |
| Diffractometer | Bruker Venture Metaljet |
| Absorption correction | Multi-scan ( |
|
| 0.570, 0.752 |
| No. of measured, independent and observed [ | 19524, 2055, 1640 |
|
| 0.073 |
| (sin θ/λ)max (Å−1) | 0.652 |
| Refinement | |
|
| 0.063, 0.183, 1.05 |
| No. of reflections | 2055 |
| No. of parameters | 168 |
| H-atom treatment | All H-atom parameters refined |
| Δρmax, Δρmin (e Å−3) | 0.35, −0.37 |
Computer programs: APEX3 and SAINT (Bruker, 2016 ▸), SHELXT (Sheldrick, 2015a ▸), SHELXL2016 (Sheldrick, 2015b ▸), OLEX2 (Dolomanov et al., 2009 ▸) and Mercury (Macrae et al., 2008 ▸).
| C9H10O5 | |
| Monoclinic, | Ga |
| Cell parameters from 9932 reflections | |
| θ = 4.0–60.8° | |
| µ = 0.65 mm−1 | |
| β = 95.804 (3)° | |
| Chunk, clear light colourless | |
| 0.11 × 0.08 × 0.08 mm |
| Bruker Venture Metaljet diffractometer | 2055 independent reflections |
| Radiation source: Metal Jet, Gallium Liquid Metal Jet Source | 1640 reflections with |
| Helios MX Mirror Optics monochromator | |
| Detector resolution: 10.24 pixels mm-1 | θmax = 60.9°, θmin = 4.0° |
| ω and φ scans | |
| Absorption correction: multi-scan (SADABS; Krause | |
| 19524 measured reflections |
| Refinement on | Hydrogen site location: difference Fourier map |
| Least-squares matrix: full | All H-atom parameters refined |
| (Δ/σ)max < 0.001 | |
| Δρmax = 0.35 e Å−3 | |
| 2055 reflections | Δρmin = −0.37 e Å−3 |
| 168 parameters | Extinction correction: SHELXL2016 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 0 restraints | Extinction coefficient: 0.0045 (17) |
| Experimental. X-ray crystallographic data for I were collected from a single crystal sample, which was mounted on a loop fiber. Data were collected using a Bruker Venture diffractometer equipped with a Photon 100 CMOS Detector, a Helios MX optics and a Kappa goniometer. The crystal-to-detector distance was 4.0 cm, and the data collection was carried out in 1024 x 1024 pixel mode. |
| 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. |
| O1 | 0.8442 (2) | 0.6986 (2) | 0.38601 (7) | 0.0450 (4) | |
| O2 | 0.8604 (2) | 0.3277 (2) | 0.44578 (7) | 0.0445 (4) | |
| O3 | 1.0103 (2) | 0.5925 (2) | 0.30315 (8) | 0.0528 (5) | |
| O4 | 0.7313 (2) | 0.4446 (2) | 0.53563 (7) | 0.0500 (4) | |
| O5 | 0.5693 (2) | 0.3519 (2) | 0.32715 (7) | 0.0433 (4) | |
| C1 | 0.8967 (3) | 0.3454 (3) | 0.37415 (10) | 0.0442 (5) | |
| H1 | 1.029 (4) | 0.277 (3) | 0.3718 (12) | 0.047 (6)* | |
| C2 | 0.9217 (3) | 0.5552 (3) | 0.35135 (10) | 0.0427 (5) | |
| C3 | 0.7092 (3) | 0.6521 (3) | 0.43558 (10) | 0.0413 (5) | |
| H3 | 0.591 (3) | 0.624 (3) | 0.4123 (11) | 0.033 (5)* | |
| C4 | 0.7669 (3) | 0.4688 (3) | 0.47711 (10) | 0.0412 (5) | |
| C5 | 0.6982 (4) | 0.8289 (4) | 0.48109 (12) | 0.0490 (6) | |
| H5A | 0.817 (4) | 0.861 (4) | 0.5017 (13) | 0.050 (6)* | |
| H5B | 0.656 (4) | 0.940 (4) | 0.4515 (14) | 0.059 (7)* | |
| H5C | 0.613 (4) | 0.797 (4) | 0.5153 (16) | 0.061 (8)* | |
| C6 | 0.7425 (3) | 0.2424 (3) | 0.32707 (12) | 0.0452 (5) | |
| H6A | 0.725 (3) | 0.111 (4) | 0.3442 (12) | 0.041 (6)* | |
| H6B | 0.783 (3) | 0.234 (3) | 0.2801 (14) | 0.047 (6)* | |
| C7 | 0.4081 (3) | 0.2573 (3) | 0.28966 (11) | 0.0472 (5) | |
| H7A | 0.299 (3) | 0.349 (3) | 0.2863 (11) | 0.041 (6)* | |
| H7B | 0.440 (3) | 0.222 (3) | 0.2426 (14) | 0.047 (6)* | |
| C8 | 0.3455 (3) | 0.0836 (3) | 0.32598 (10) | 0.0437 (5) | |
| C9 | 0.2952 (3) | −0.0550 (3) | 0.35607 (12) | 0.0476 (5) | |
| H9 | 0.252 (4) | −0.157 (4) | 0.3776 (15) | 0.060 (8)* |
| O1 | 0.0527 (9) | 0.0485 (8) | 0.0346 (8) | −0.0021 (6) | 0.0088 (6) | 0.0033 (6) |
| O2 | 0.0478 (8) | 0.0505 (8) | 0.0355 (8) | 0.0025 (6) | 0.0065 (6) | 0.0062 (6) |
| O3 | 0.0586 (9) | 0.0640 (10) | 0.0373 (8) | −0.0117 (7) | 0.0125 (7) | −0.0011 (7) |
| O4 | 0.0548 (9) | 0.0617 (9) | 0.0338 (8) | −0.0022 (7) | 0.0066 (6) | 0.0060 (6) |
| O5 | 0.0446 (8) | 0.0472 (8) | 0.0383 (8) | −0.0030 (6) | 0.0057 (6) | −0.0039 (6) |
| C1 | 0.0453 (11) | 0.0522 (12) | 0.0367 (11) | 0.0023 (9) | 0.0119 (9) | 0.0025 (8) |
| C2 | 0.0436 (11) | 0.0538 (12) | 0.0310 (10) | −0.0062 (9) | 0.0050 (8) | 0.0003 (8) |
| C3 | 0.0411 (10) | 0.0519 (11) | 0.0311 (9) | 0.0003 (9) | 0.0048 (8) | 0.0023 (8) |
| C4 | 0.0392 (10) | 0.0520 (11) | 0.0321 (10) | −0.0041 (8) | 0.0028 (8) | 0.0017 (8) |
| C5 | 0.0534 (13) | 0.0552 (13) | 0.0380 (11) | 0.0041 (10) | 0.0035 (10) | −0.0019 (9) |
| C6 | 0.0521 (12) | 0.0463 (11) | 0.0390 (11) | 0.0015 (9) | 0.0128 (9) | −0.0016 (8) |
| C7 | 0.0511 (12) | 0.0557 (12) | 0.0344 (10) | −0.0038 (10) | 0.0026 (9) | −0.0012 (9) |
| C8 | 0.0445 (11) | 0.0535 (12) | 0.0327 (10) | −0.0027 (9) | 0.0019 (8) | −0.0055 (8) |
| C9 | 0.0503 (12) | 0.0507 (12) | 0.0419 (11) | −0.0062 (10) | 0.0049 (9) | −0.0031 (9) |
| O1—C2 | 1.335 (3) | C3—C4 | 1.522 (3) |
| O1—C3 | 1.451 (2) | C3—C5 | 1.505 (3) |
| O2—C1 | 1.449 (3) | C5—H5A | 0.91 (3) |
| O2—C4 | 1.344 (3) | C5—H5B | 0.98 (3) |
| O3—C2 | 1.203 (3) | C5—H5C | 0.96 (3) |
| O4—C4 | 1.203 (3) | C6—H6A | 0.97 (2) |
| O5—C6 | 1.421 (3) | C6—H6B | 0.99 (3) |
| O5—C7 | 1.432 (3) | C7—H7A | 0.98 (2) |
| C1—H1 | 1.04 (2) | C7—H7B | 1.00 (3) |
| C1—C2 | 1.515 (3) | C7—C8 | 1.470 (3) |
| C1—C6 | 1.515 (3) | C8—C9 | 1.184 (3) |
| C3—H3 | 0.92 (2) | C9—H9 | 0.88 (3) |
| C2—O1—C3 | 119.98 (16) | C3—C5—H5A | 110.8 (16) |
| C4—O2—C1 | 121.22 (16) | C3—C5—H5B | 107.6 (15) |
| C6—O5—C7 | 112.74 (16) | C3—C5—H5C | 107.4 (16) |
| O2—C1—H1 | 104.3 (14) | H5A—C5—H5B | 106 (2) |
| O2—C1—C2 | 113.46 (17) | H5A—C5—H5C | 110 (2) |
| O2—C1—C6 | 111.23 (18) | H5B—C5—H5C | 115 (2) |
| C2—C1—H1 | 106.6 (13) | O5—C6—C1 | 107.90 (17) |
| C6—C1—H1 | 110.0 (13) | O5—C6—H6A | 110.3 (13) |
| C6—C1—C2 | 110.91 (17) | O5—C6—H6B | 111.0 (14) |
| O1—C2—C1 | 118.72 (18) | C1—C6—H6A | 109.2 (13) |
| O3—C2—O1 | 120.44 (19) | C1—C6—H6B | 109.7 (14) |
| O3—C2—C1 | 120.83 (19) | H6A—C6—H6B | 108.8 (19) |
| O1—C3—H3 | 109.1 (13) | O5—C7—H7A | 108.0 (13) |
| O1—C3—C4 | 112.30 (16) | O5—C7—H7B | 109.8 (14) |
| O1—C3—C5 | 106.96 (18) | O5—C7—C8 | 112.01 (17) |
| C4—C3—H3 | 105.6 (13) | H7A—C7—H7B | 109.8 (18) |
| C5—C3—H3 | 111.0 (13) | C8—C7—H7A | 106.4 (13) |
| C5—C3—C4 | 111.88 (17) | C8—C7—H7B | 110.8 (13) |
| O2—C4—C3 | 117.51 (17) | C9—C8—C7 | 179.1 (2) |
| O4—C4—O2 | 119.26 (18) | C8—C9—H9 | 177.3 (19) |
| O4—C4—C3 | 123.22 (19) | ||
| O1—C3—C4—O2 | −31.7 (2) | C3—O1—C2—O3 | 168.81 (18) |
| O1—C3—C4—O4 | 149.05 (19) | C3—O1—C2—C1 | −11.5 (3) |
| O2—C1—C2—O1 | −23.6 (3) | C4—O2—C1—C2 | 30.6 (3) |
| O2—C1—C2—O3 | 156.06 (19) | C4—O2—C1—C6 | −95.2 (2) |
| O2—C1—C6—O5 | 70.2 (2) | C5—C3—C4—O2 | −152.00 (19) |
| C1—O2—C4—O4 | 176.43 (18) | C5—C3—C4—O4 | 28.8 (3) |
| C1—O2—C4—C3 | −2.8 (3) | C6—O5—C7—C8 | 71.3 (2) |
| C2—O1—C3—C4 | 39.0 (2) | C6—C1—C2—O1 | 102.4 (2) |
| C2—O1—C3—C5 | 162.14 (17) | C6—C1—C2—O3 | −77.9 (2) |
| C2—C1—C6—O5 | −57.0 (2) | C7—O5—C6—C1 | −174.10 (17) |
| H··· | ||||
| C3—H3···O4i | 0.92 (2) | 2.60 (2) | 3.247 (3) | 127.8 (16) |
| C3—H3···O5 | 0.92 (2) | 2.49 (2) | 3.033 (2) | 118.1 (16) |
| C6—H6 | 0.99 (3) | 2.47 (2) | 3.369 (3) | 151.0 (19) |
| C7—H7 | 0.98 (2) | 2.66 (2) | 3.627 (3) | 169.1 (18) |
| C9—H9···O4iv | 0.88 (3) | 2.58 (3) | 3.412 (3) | 156 (2) |