Heat capacity of NH4Cl1 − xBrx solid solutions in the vicinity of the γ-to-β phase transition

1984 ◽  
Vol 16 (8) ◽  
pp. 719-732 ◽  
Author(s):  
E.B. Amitin ◽  
O.A. Nabutovskaya ◽  
I.E. Paukov ◽  
K.S. Sukhovey
1985 ◽  
Vol 54 (2) ◽  
pp. 625-629 ◽  
Author(s):  
Masahide Matsuura ◽  
Haruhiko Yao ◽  
Kazutoshi Gouhara ◽  
Ichiro Hatta ◽  
Norio Kato

The heat capacity of the mixed crystals NH 4 Br 0.20 CI 0.80 and NH 4 Br 0.74 CI 0.26 has been measured from ca . 8 to 300 K. The first of these solids has, as expected, two gradual transitions, the lower having an entropy of transition ∆ S λ of 3.79 J K –1 mol –1 , and the upper a ∆ S λ of 4.51 J K –1 mol –1 . The heat capacity between these two transitions is always considerably above the ‘normal’ or baseline value, and it appears that the orientational disordering of the ammonium ions, while completed in the γ → β transition, commences in the δ-phase. The other, bromide-rich mixed crystal shows no sign of a δ → γ transition, but has a λ -type γ → β transition which culminates at 262.5 K, with ∆ S λ = 7.31 J K –1 mol –1 . The heat capacity of both mixed crystals in the β-phase, like that of the pure components, is ‘anomalously’ high, the additional heat capacity for the solid solutions being larger than that for the pure salts. The phase diagram for the ammonium-chloride–ammonium-bromide system is shown; it combines previous information with that provided by the heat-capacity results reported in this and previous papers.


2008 ◽  
Vol 587-588 ◽  
pp. 114-117 ◽  
Author(s):  
V.V. Murasheva ◽  
Elena A. Fortalnova ◽  
Ekaterina D. Politova ◽  
Marina G. Safronenko ◽  
Sergei Yu. Stefanovich ◽  
...  

The polymorph phase stability ranges have been studied for the Bi4V2-xMexO11-y solid solutions with Me = Ga and Zr at room temperature. The formation of orthorhombic α- (x = 0.0 and 0.05) and β-phases (x = 0.1, 0.15) and tetragonal phase (0.2 ≤ x ≤ 0.3) has been revealed in BIGAVOX solid solutions. In BIZRVOX solid solutions, α-phase exists at x ≤ 0.05, while β-phase exists at 0.1 ≤ x ≤ 0.3. The second order phase transitions at ~ 308°C (BIGAVOX) and ~ 270°C (BIZRVOX) have been revealed for solid solutions with x = 0.05 using the SHG and DSC methods. In both systems, the β↔γ-phase transition temperatures have been found to decrease with increasing x.


2013 ◽  
Vol 32 (2) ◽  
pp. 189-194 ◽  
Author(s):  
H. Yurtseven ◽  
M. Desticioğlu

AbstractThe α-β transition (TQ = 578°C) is studied in quartz by analyzing the experimental heat capacity Cp data taken from the literature, using a power-law formula. Values of the critical exponent α for Cp are extracted below and above TQ, which describe the α-β transition as a second order transition in quartz. The α values obtained here are compared with the predictions of the theoretical models.


1988 ◽  
Vol 66 (4) ◽  
pp. 549-552 ◽  
Author(s):  
Jane E. Callanan ◽  
Ron D. Weir ◽  
Edgar F. Westrum Jr.

We have measured the heat capacity of the fast ion conductor PbSnF4 at 10.3 < T < 352 K by adiabatic calorimetry. Our results show anomalous values in the Cp,m in the region 300 < T < 352 K. These are associated with the α–β crystallographic transition reported at 353 K. Because the upper temperature limit of our cryostat is around 354 K, it was impossible to follow the phase transition to completion. A more subtle anomaly in the Cp,m was detected between 130 and 160 K. Standard molar thermodynamic functions are presented at selected temperatures from 5 to 350 K.


2000 ◽  
Vol 42 (1) ◽  
pp. 161-164 ◽  
Author(s):  
I. P. Raevskii ◽  
V. V. Eremkin ◽  
V. G. Smotrakov ◽  
E. S. Gagarina ◽  
M. A. Malitskaya

Nano Energy ◽  
2021 ◽  
Vol 89 ◽  
pp. 106474
Author(s):  
Mengde Zhu ◽  
Siqi Li ◽  
Hongfang Zhang ◽  
Ju Gao ◽  
K.W. Kwok ◽  
...  

2009 ◽  
Vol 51 (3) ◽  
pp. 589-592 ◽  
Author(s):  
L. I. Isaenko ◽  
S. V. Mel’nikova ◽  
A. A. Merkulov ◽  
V. M. Pashkov ◽  
A. Yu. Tarasova

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