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FeAs: Heat capacity, enthalpy increments, other thermodynamic properties from 5 to 1350 K, and magnetic transition
The heat capacity of iron monoarsenide has been determined by adiabatic calorimetry from 5 to 1030 K and by drop calorimetry relative to 298.15 K over the range 875 to 1350 K. A small λ-type transition is observed at T N = (70.95±0.02) K. It is related to the disappearance of a doubly helically orde...
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Published in: | The Journal of chemical thermodynamics 1989-04, Vol.21 (4), p.363-373 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The heat capacity of iron monoarsenide has been determined by adiabatic calorimetry from 5 to 1030 K and by drop calorimetry relative to 298.15 K over the range 875 to 1350 K. A small λ-type transition is observed at
T
N = (70.95±0.02) K. It is related to the disappearance of a doubly helically ordered magnetic-spin structure on heating. The obviously cooperative entropy increment of transition is only
Δ
trs
S
m
o
R = 0.021
. The higher-temperature heat capacity rises considerably above lattice expectations. Part of the rise is ascribed to low-spin electron redistribution in iron, while the further excess above 800 K presumably arises from a beginning low- to high-spin transition, possibly connected with interstitial defect formation in the MnP-type structure. FeAs melts at about 1325 K with
Δ
fus
H
m
o = 6180
R · K. Thermodynamic functions have been evaluated and the values of
C
p, m
(
T),
S
m
o(
T),
H
m
o(
T), and
Φ
m
o(
T), are 6.057
R, 7.513
R, 1177
R · K, and 3.567
R at 298.15 K, and 8.75
R, 16.03
R · K, and 9.745
R at 1000 K. |
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ISSN: | 0021-9614 1096-3626 |
DOI: | 10.1016/0021-9614(89)90137-7 |