The temperature dependences of the molar heat capacities of \(\mathrm{CuTeO}_{3}, \mathrm{CuTe}_{2} \mathrm{O}_{5}\), and \(\mathrm{CuO} \cdot \mathrm{CuTeO}_{3}\) were determined. By statistical manipulation of the values obtained, the parameters in the equations for the corresponding compounds wer
Low-temperature heat capacity of sodium borosilicate glasses at temperatures from 13 K to 300 K
β Scribed by Isao Yamashita; Takeo Tojo; Hitoshi Kawaji; Tooru Atake; Yannick Linard; Pascal Richet
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 158 KB
- Volume
- 33
- Category
- Article
- ISSN
- 0021-9614
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β¦ Synopsis
Thermodynamic properties of sodium borosilicate glasses {56.7 SiO 2 , (43.7 -x) B 2 O 3 , xNa 2 O} where x = 14.4, 22.9, and 32.5, have been studied. The heat capacity was measured using an adiabatic calorimeter at temperatures between 13 K and 300 K. The thermodynamic functions were calculated from the smoothed values of C p,m . The results differ from an additive model with pure glassy SiO 2 , B 2 O 3 , and crystalline Na 2 O as components. A model based on the assumption that the contribution of structural units of glasses to the heat capacity is equal to those of glasses with the same molecular formula is proposed.
π SIMILAR VOLUMES
The heat capacity of manganese monophosphide MnP has been determined by adiabatic shield calorimetry at temperatures from 5 K to 840 K. The heli-to ferromagnetic transition is noted only as a slightly enhanced heat capacity at T f 53 K. A -type heat capacity contribution with maximum at T s 289.5 K
The heat capacity of synthetic Cu3AsS4 (enargite) was measured by quasi-adiabatic calorimetry from the temperatures 5 K to 355 K and by differential scanning calorimetry from T=339 K to T=720 K. Heat-capacity anomalies were observed at T=(58.520.5) The causes of the anomalies are unknown. At T=298.