Brás Ana R, Noronha João P, Antunes Alexandra M M, Cardoso Maria M, Schönhals Andreas, Affouard Frédéric, Dionísio Madalena, Correia Natália T
Requimte, Departamento de Química, Faculdade de Ciências e Tecnologia, Universidade Nova de Lisboa, 2829-516 Caparica, Portugal.
J Phys Chem B. 2008 Sep 4;112(35):11087-99. doi: 10.1021/jp8040428. Epub 2008 Aug 8.
The molecular mobility of amorphous ibuprofen has been investigated by broadband dielectric relaxation spectroscopy (DRS) covering a temperature range of more than 200 K. Four different relaxation processes, labeled as alpha, beta, gamma, and D, were detected and characterized, and a complete relaxation map was given for the first time. The gamma-process has activation energy E a = 31 kJ.mol (-1), typical for local mobility. The weak beta-relaxation, observed in the glassy state as well as in the supercooled state was identified as the genuine Johari-Goldstein process. The temperature dependence of the relaxation time of the alpha-process (dynamic glass transition) does not obey a single VFTH law. Instead two VFTH regimes are observed separated by a crossover temperature, T B = 265 K. From the low temperature VFTH regime, a T g (diel) (tau =100 s) = 226 K was estimated, and a fragility or steepness index m = 93, was calculated showing that ibuprofen is a fragile glass former. The D-process has a Debye-like relaxation function but the temperature dependence of relaxation time also follows the VFTH behavior, with a Vogel temperature and a pre-exponential factor which seem to indicate that its dynamics is governed by the alpha-process. It has similar features as the Debye-type process observed in a variety of associating liquids, related to hydrogen bonding dynamics. The strong tendency of ibuprofen to form hydrogen bonded aggregates such as dimers and trimers either cyclic or linear which seems to control in particular the molecular mobility of ibuprofen was confirmed by IR spectroscopy, electrospray ionization mass spectrometry, and MD simulations.
通过覆盖超过200 K温度范围的宽带介电弛豫谱(DRS)研究了非晶态布洛芬的分子迁移率。检测并表征了四种不同的弛豫过程,分别标记为α、β、γ和D,并首次给出了完整的弛豫图谱。γ过程的活化能E a = 31 kJ·mol⁻¹,这是局部迁移率的典型值。在玻璃态以及过冷态中观察到的弱β弛豫被确定为真正的乔哈里 - 戈尔茨坦过程。α过程(动态玻璃化转变)的弛豫时间的温度依赖性并不遵循单一的VFTH定律。相反,观察到两个VFTH区域,由交叉温度T B = 265 K分隔。从低温VFTH区域估计出T g (diel)(τ = 100 s)= 226 K,并计算出脆性或陡度指数m = 93,表明布洛芬是一种脆性玻璃形成体。D过程具有类似德拜的弛豫函数,但弛豫时间的温度依赖性也遵循VFTH行为,其Vogel温度和预指数因子似乎表明其动力学受α过程支配。它具有与在各种缔合液体中观察到的德拜型过程相似的特征,与氢键动力学有关。红外光谱、电喷雾电离质谱和分子动力学模拟证实了布洛芬强烈倾向于形成氢键聚集体,如环状或线性的二聚体和三聚体,这似乎特别控制了布洛芬的分子迁移率。