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
Heat capacity and thermodynamic properties of anisotropic crystals: PbI2, ZnCl2, and AsI3at temperatures from 5 K to 350 K
β Scribed by J.T Sipowska; J.J McBride; E.F Westrum; Jr
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 175 KB
- Volume
- 30
- Category
- Article
- ISSN
- 0021-9614
No coin nor oath required. For personal study only.
β¦ Synopsis
Heat capacities of PbI , ZnCl , and AsI have been determined by adiabatic shield 2 2 3 calorimetry from T s 5 K to T s 350 K. No anomalous regions were found in the heat capacity of PbI and ZnCl . Two anomalous regions were found in the heat capacity of AsI : 2 2 3 one small sharp peak at T s 161 K, and the other, a broad region from about T s 225 K to T s 290 K. The thermodynamic properties have been evaluated and the values of molar heat capacity, entropy, and enthalpy at T s 298.
π SIMILAR VOLUMES
The heat capacity of ammonium hexabromotellurate (NH4)2TeBr6 was measured at temperatures from T = 5 K to T = 345 K by adiabatic calorimetry. Two l-shaped transitions were present, one at T = (193.25 2 0.05) K, with DtrsSΒ°m = (1.145 2 0.010)β’R, and another at T = (212.2 2 0.2) K, with DtrsSΒ°m = (0.1
The heat capacity of tungsten disilicide \(\mathrm{WSi}_{2.06}\) was measured over the temperature range \(5.9<(T / K)<341\) using adiabatic calorimetry. Our results show that neither a phase transition nor anomalies are present. A contribution from the electronic molar heat capacity is present and
The molar heat capacity of ammonium hexafluorogermanate NH GeF was measured 4 2 6 from T f 5 K to T s 326 K by adiabatic calorimetry. Our results show that neither a transition nor the metastability that sometimes occurs in R MX compounds was present. 2 6 T 0 ΓΕ½ . 4 Ε½ . From our results, the standar