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Simple practical system for directly measuring magnetocaloric effects under large magnetic fields
Direct measurements of the adiabatic temperature change (ΔTad) in Gd and Mn1.15Fe0.8P0.5Si0.5C0.05 are made using a homemade adiabatic magnetocalorimeter at 260–360 K and 0–7 T. The system uses a servo motor to drive the samples into and out of the magnetic field under a vacuum environment provided...
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Published in: | Review of scientific instruments 2020-06, Vol.91 (6), p.065102-065102 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Direct measurements of the adiabatic temperature change
(ΔTad) in Gd and
Mn1.15Fe0.8P0.5Si0.5C0.05 are
made using a homemade adiabatic magnetocalorimeter at 260–360 K and 0–7 T. The system uses
a servo motor to drive the samples into and out of the magnetic field under a vacuum
environment provided by the Physical Property Measurement System (PPMS). The peak values
of ΔTad for Gd and
Mn1.15Fe0.8P0.5Si0.5C0.05 at 7 T
are 8.71 K and 6.41 K at ambient temperatures of 303 K and 317 K, respectively. Based on
the theory model, it is found that ΔTad of Gd depends on the
2/3 exponential function of magnetic field H
(ΔTad ∝ H2/3), whereas the
Mn1.15Fe0.8P0.5Si0.5C0.05
compound follows the power law of ΔTad ∝
H0.66–1.04 due to the first order magnetic transitions.
Furthermore, using the constructed experimental instrument, the adiabatic temperature
change in different magnetic materials, including materials with first/second order
magnetic transition and blocks, flakes, or powders, can be directly measured under large
magnetic fields and wide temperature spans. |
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ISSN: | 0034-6748 1089-7623 |
DOI: | 10.1063/1.5128949 |