Ion Dranca/Chem.J. Mold. 2008, 3 (1), 31-43Table 1Size <strong>of</strong> Cooperatively Rearranging Region and Experimental Parameters Used for Its Calculationssample T g, K C pg,J K -1 g -1 C pl, J K -1 g -1 T,K V g,nm 3PS100 366.9 1.53 1.87 2.6 20.9nPS90 379.4 1.45 1.69 1.9 36.7It is seen that the Cp values for the PS-clay system are noticeably smaller than for virgin PS. The decreasecannot be explained by the simply presence <strong>of</strong> clay because it is present in a very small amount (1%) and its heatcapacity [65] is comparable to that <strong>of</strong> PS. On the other hand, the value <strong>of</strong> heat capacity is proportional to the number<strong>of</strong> internal degrees <strong>of</strong> freedom <strong>of</strong> molecular motion. By applying 7-10 to the heat capacity data (Fig. 5), we have1/3evaluated the volume <strong>of</strong> cooperatively rearranging region PS100 and nPS90 (Table 1). The values ( V g) givesthe characteristic length <strong>of</strong> the cooperatively rearranging region [48, 60]. According to our data for PS100 (Table 1), is 2.8 nm, which agrees well with the value 3.0 nm recently reported by Hempel et al. [62].Glass transition or -relaxation in Indomethacin. By applying the isoconversional method [49, 50] to the versus T data for different heating rates, [46] we obtained the E dependence shown in Fig. 6.350300E / kJ mol -12502001500.0 0.2 0.4 0.6 0.8 1.0Fig. 6. Variation <strong>of</strong> the activation energy for the -relaxation with the extent <strong>of</strong> relaxationfor the glass transition in indomethacinThe effective activation energy decreases from 320 to 160 kJ mol -1 . A decrease in E with the transition from the glassyto liquid state has also been reported by Hancock et al. [66], who estimated E for the onset, midpoint, and <strong>of</strong>fset <strong>of</strong> thetransition, and obtained respective values <strong>of</strong> 385, 263, and 190 kJ mol. -1The decrease in E can be explained in terms <strong>of</strong> cooperative molecular motion. The glassy state has a smallamount <strong>of</strong> free volume that permits only the local motion (i.e., the -process) (Fig. 1) that persists well below the glasstransition temperature. As the temperature increases and approaches the region <strong>of</strong> the glass transition, the molecularmotion becomes more intense, and the free volume rises, initiating the -process. This process needs a great degree<strong>of</strong> cooperativity between the molecules, which gives rise to a large energy barrier represented by a large value <strong>of</strong>E at the initial stage <strong>of</strong> transition. As the free volume grows with increasing temperature, the molecular packingbecomes looser, allowing molecules to relax more independently (i.e., with a smaller degree <strong>of</strong> cooperativity). Asa result, the energetic constraints relax, and the effective activation energy drops. Note that a fall <strong>of</strong> E is consistentwith both the WLF and VTF equations [12-15]. A decrease is also predicted by the Adam-Gibs equation [67].z Aexp()k TB(11)37
Ion Dranca/Chem.J. Mold. 2008, 3 (1), 31-43where kBis the Boltzman constant, is the activation energy per particle, and z * is the number <strong>of</strong> particles thatrearrange cooperatively. In eq 11, z is inversely proportional to the configurational entropy that rises with T, so thatboth z * and the effective activation energy (i.e., z * ) decrease with increasing T.Size <strong>of</strong> Cooperatively Rearranging Regions in Indomethacin. Figure 7 shows a C pversus T curve that is anaverage <strong>of</strong> three independent measurements.1.81.61.5684%C p/ J K -1 g -11.41.216%T=5.01.191.00 20 40 60 80T / o CFig. 7. Temperature dependence <strong>of</strong> the heat capacity for indomethacin. The heat capacity at the glasstransition (319 K) changes from 1.19 to 1.56 K -1 g -1 . T is determined as the temperature intervalin which C pchanges from 16 to 84% <strong>of</strong> the total C pThe obtained C pdata agree very well with the earlier measurements [68]. The application <strong>of</strong> eqs 7-10 to theC pdata (Figure 6) yields the volume <strong>of</strong> the cooperatively rearranging region <strong>of</strong> 40.5 nm 3 . The characteristic length<strong>of</strong> the cooperatively rearranging region (Figure 1) or the average distance between the mobility islands [42] estimatedas =(V ) 1/3 is 3.4 nm. The value is comparable to that estimated for sorbitol, 3.6 nm [62] .The numbers <strong>of</strong> moleculesinvolved in the cooperatively rearranging region is determined asN2 1RTg(Cv) (12)2M ( T)where R is the gas constant and M =357.8 g mol -1 is the molecular weight <strong>of</strong> indomethacin. The resulting value is ~90molecules.Glass transition or -relaxation in Glucose and Maltitol. Heating glassy maltitol and glucose throughout thetemperature region <strong>of</strong> the glass transition results in obtaining typical step-like DSC traces (Fig.8).-0.51.5Heat flow / W -1g-0.6-0.7-0.8-0.9-1.0exo-0 20 40 60 80 100T / o CFig. 8. DSC curves and normalized heat capacities for the glass transition <strong>of</strong> maltitol (circles)and glucose (squares) at 20 o C min -1 . Prior to heating the samples were heated ~40 o C above their T g,held at this temperature for 10 min, and cooled down to ~40oC below T gwithout aging1.00.50.0C pN38
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