Loading…

Optimal temperature range for determining magnetocaloric magnitudes from heat capacity

The determination of the magnetocaloric magnitudes (specific magnetic entropy change, ΔsM, and adiabatic temperature change, ΔTad) from heat capacity (cH) measurements requires measurements performed at very low temperatures (~0 K) or data extrapolation when the low temperature range is unavailable....

Full description

Saved in:
Bibliographic Details
Published in:Journal of physics. D, Applied physics Applied physics, 2016-12, Vol.49 (49), p.495001
Main Authors: Moreno-Ramírez, L M, Blázquez, J S, Law, J Y, Franco, V, Conde, A
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:The determination of the magnetocaloric magnitudes (specific magnetic entropy change, ΔsM, and adiabatic temperature change, ΔTad) from heat capacity (cH) measurements requires measurements performed at very low temperatures (~0 K) or data extrapolation when the low temperature range is unavailable. In this work we analyze the influence on the calculated ΔsM and ΔTad of the usually employed linear extrapolation of cH from the initial measured temperature down to 0 K. Numerical simulations have been performed using the Brillouin equation of state, the Debye model and the Fermi electron statistics to reproduce the magnetic, lattice and electronic subsystems, respectively. It is demonstrated that it is not necessary to reach experimentally temperatures very close to 0 K due to the existence of certain starting temperatures of the experiments, the same for ΔsM and ΔTad, that minimize the error of the results. A procedure is proposed to obtain the experimental magnitudes of ΔsM and ΔTad with a minimum error from cH data limited in temperature. It has been successfully applied to a GdZn alloy and results are compared to those derived from magnetization measurements.
ISSN:0022-3727
1361-6463
DOI:10.1088/0022-3727/49/49/495001