Structural and vibrational characterization of methyl glycolate in the lowtemperature crystalline and glassy states

Citation
S. Jarmelo et al., Structural and vibrational characterization of methyl glycolate in the lowtemperature crystalline and glassy states, PHYS CHEM P, 2(6), 2000, pp. 1155-1163
Citations number
30
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
PHYSICAL CHEMISTRY CHEMICAL PHYSICS
ISSN journal
14639076 → ACNP
Volume
2
Issue
6
Year of publication
2000
Pages
1155 - 1163
Database
ISI
SICI code
1463-9076(2000)2:6<1155:SAVCOM>2.0.ZU;2-A
Abstract
The low temperature phases of methyl glycolate (MGly) were identified and c haracterized structurally by differential scanning calorimetry, infrared an d Raman spectroscopies and molecular modeling. Within the temperature range 13-273 K, MGly may exist in three solid phases. A crystalline phase (I) ca n be formed from the liquid upon slow cooling [T-onset=222-227 K] or from t he low temperature glassy state resulting from fast deposition of the vapou r onto a cold substrate at 13 K and subsequent warming. A mixture of the gl assy state and crystalline phase (I) is obtained by cooling the liquid at h igher cooling rates (v(cooling)greater than or equal to 10 K min(-1)). Upon heating this mixture, devitrification occurs at ca. 175 K, the cold liquid then formed giving rise to a second crystalline variety (II) at T-onset=19 8-207 K. In the glassy state, individual MGly molecules may assume the two conformational states previously observed for this compound isolated in an argon matrix and in the liquid phase [S. Jarmelo and R. Fausto, J. Mol. Str uct., 1999, 509, 183]. On the contrary, the crystalline phase I was found t o exhibit conformational selectivity-in this phase, all individual molecule s assume a conformation analogous to the most stable conformer found for th e isolated molecule and in the liquid (the syn-syn s-cis conformer, where t he H-O-C-C, O-C-C=O and O=C-O-C dihedrals are ca. 0 degrees). In agreement with the spectroscopic results, a molecular modeling analysis reveals that, in this phase, two non-equivalent molecules exhibiting an intramolecular O H ... O=hydrogen bond exist, which are connected by a relatively strong int ermolecular OH ... O'2=hydrogen bond. Crystalline state II could not be cha racterized in detail structurally, but the thermodynamic studies seem to in dicate that it corresponds to a metastable crystalline form having a more r elaxed structure and a slightly higher energy than crystalline state I. The observed temperature of fusion for the two observed crystalline forms are: I, 264 K and II, 260 K.