Wojnarowska Z, Adrjanowicz K, Wlodarczyk P, Kaminska E, Kaminski K, Grzybowska K, Wrzalik R, Paluch M, Ngai K L
Institute of Physics, Silesian University, ul. Uniwersytecka 4, 40-007 Katowice, Poland.
J Phys Chem B. 2009 Sep 17;113(37):12536-45. doi: 10.1021/jp905162r.
Broadband dielectric measurements on the pharmaceutical indomethacin (IMC) were performed at ambient and elevated pressure. Data on molecular dynamics collected at ambient pressure are in good agreement with that published in the literature. In the glassy state, there is a well-resolved secondary relaxation with Arrhenius activation energy E(a) = 38 kJ/mol. This commonly observed relaxation process (labeled gamma) is of intramolecular origin because it is pressure-insensitive. Closer analysis of the ambient pressure dielectric spectra obtained in the vicinity of the T(g) indicated the presence of one more secondary relaxation (beta), which is slower than that commonly observed. Application of the CM predictions enabled us to classify it as a true JG relaxation. Pressure measurements confirmed our supposition concerning the origins of the two secondary relaxations in IMC. Moreover, we have found that IMC under pressure does not crystallize, even at very high temperatures of T > or = 372 K. This finding was discussed in the framework of the two-order parameter model proposed by Tanaka (Konishi, T.; Tanaka, H. Phys. Rev B 2007, 76, 220201), as well as the JG relaxation proposal by Oguni (Hikima T.; Hanaya M.; Oguni M. J. Mol Struct. 1999, 479, 245). We also showed that the shape of the alpha-relaxation loss peak is the same when comparing dielectric spectra with the same tau(alpha) but obtained at ambient and elevated pressure. Additionally, we found out that the fragility of IMC decreases with increasing pressure. In addition, the pressure coefficient of the glass transition temperature, dT(g)/dP, was determined, and it is 255 K/GPa. Finally, we discuss the possibility of preparation of the amorphous state with higher density than by cooling of the liquid.
在室温和高压下对药物吲哚美辛(IMC)进行了宽带介电测量。在室温下收集的分子动力学数据与文献中发表的数据高度吻合。在玻璃态下,存在一个解析良好的二级弛豫,其阿仑尼乌斯活化能E(a)=38kJ/mol。这个普遍观察到的弛豫过程(标记为γ)起源于分子内,因为它对压力不敏感。对在玻璃化转变温度(Tg)附近获得的室温介电谱进行更仔细的分析表明,还存在另一个二级弛豫(β),它比通常观察到的弛豫要慢。应用CM预测使我们能够将其归类为真正的JG弛豫。压力测量证实了我们关于IMC中两个二级弛豫起源的推测。此外,我们发现,即使在T≥372K的非常高的温度下,IMC在压力下也不会结晶。在田中提出的双序参量模型(小西,T.;田中,H.《物理评论B》2007年,76,220201)以及小串提出的JG弛豫建议(日置,T.;花屋,M.;小串,M.《分子结构杂志》1999年,479,245)的框架内讨论了这一发现。我们还表明,当比较具有相同α弛豫时间(τα)但在室温和高压下获得的介电谱时,α弛豫损耗峰的形状是相同的。此外,我们发现IMC的脆性随压力增加而降低。此外,还确定了玻璃化转变温度的压力系数dTg/dP,其值为255K/GPa。最后,我们讨论了制备密度高于通过液体冷却得到的非晶态的可能性。