The apparent molar heat capacities and apparent molar volumes of Nd(ClO4)3(aq), Eu(ClO4)3(aq), Er(ClO4)3(aq), and Yb(ClO4)3(aq) have been measured at the temperatures T = (283.2, 298.2, 313.2, and 328.2) K and molalities from 10.05 molโขkg -1 to 10.7 molโขkg -1 in a Picker flow microcalorimeter and vi
Apparent molar heat capacities and volumes of LaCl3(aq), La(ClO4)3(aq), and Gd(ClO4)3(aq) between the temperatures 283 K and 338 K
โ Scribed by Caibin Xiao; Peter R. Tremaine
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 568 KB
- Volume
- 28
- Category
- Article
- ISSN
- 0021-9614
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โฆ Synopsis
The apparent molar heat capacities and volumes of LaCl3(aq), La(ClO4)3(aq), and Gd(ClO4)3(aq) have been measured at the temperatures (283, 298, 313, 328 and 338) K and molalities from about 0.05 molโขkg -1 to 0.7 molโขkg -1 in a Picker flow microcalorimeter and a vibrating tube densitometer. The results were analyzed by means of the Pitzer equations to derive standard partial molar heat capacities and volumes and expressions for the excess properties. The revised Helgeson-Kirkham-Flowers (HKF) model has been found to represent the temperature dependence of the standard partial molar properties within the experimental uncertainty. A modification to the non-electrostatic heat capacity function in the HKF model yields an improved fit to the experimental results for La(ClO4)3 and Gd(ClO4)3.
๐ SIMILAR VOLUMES
The apparent molar heat capacities C โข p,ฯ and apparent molar volumes V โข ฯ of Y 2 (SO 4 ) 3 (aq), La 2 (SO 4 ) 3 (aq), Pr 2 (SO 4 ) 3 (aq), Nd 2 (SO 4 ) 3 (aq), Eu 2 (SO 4 ) 3 (aq), Dy 2 (SO 4 ) 3 (aq), Ho 2 (SO 4 ) 3 (aq), and Lu 2 (SO 4 ) 3 (aq) were measured at T = 298.15 K and p = 0.1 MPa with