Influence of a Cyclic Magnetic Field on the Direct and Inverse Magnetocaloric Effects in the Ni44Co6Mn32Al18 Heusler Ribbon

The results of direct measurements for the adiabatic temperature change ∆Tad in a rapidly quenched ribbons Heusler Ni44Co6Mn32Al18 alloy specimen within a temperature range of 100–350 K in a cyclic magnetic field with a strength of 18 kOe and a frequency of 0.2 Hz are presented. It is shown that, in the case of one-time magnetic field actuation, the inverse effect value is –0.25 K at a magnetostructural transition temperature TS. The second and following on/off cycles lead to a decrease in the effect by an order of magnitude to –0.03 K. Such a behavior is associated with the effect of kinetic relaxation in the martensite phase and phase transition irreversibility in the used magnetic fields. Near TC, the stable and direct effect ∆Tad = 0.23 K without degradation signs is observed.

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Publication Details

Journal
The Physics of Metals and Metallography
Published
2024-12-01
DOI
https://doi.org/10.1134/s0031918x24602361
Citations
3
Primary Topic
Shape Memory Alloy Transformations
Type
article
Field-Weighted Citation Impact
0.35
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article

Influence of a Cyclic Magnetic Field on the Direct and Inverse Magnetocaloric Effects in the Ni44Co6Mn32Al18 Heusler Ribbon

A. M. Aliev, Nguyen Huy Dan, Anvar Kadirbardeev, A. G. Gamzatov et al.
3 citations
The Physics of Metals and Metallography
Shape Memory Alloy Transformations
0.35
article

Influence of a Cyclic Magnetic Field on the Direct and Inverse Magnetocaloric Effects in the Ni44Co6Mn32Al18 Heusler Ribbon

A. M. Aliev, Nguyen Huy Dan, Anvar Kadirbardeev, A. G. Gamzatov, N. H. Yen
article en
3 citations

Abstract

The results of direct measurements for the adiabatic temperature change ∆Tad in a rapidly quenched ribbons Heusler Ni44Co6Mn32Al18 alloy specimen within a temperature range of 100–350 K in a cyclic magnetic field with a strength of 18 kOe and a frequency of 0.2 Hz are presented. It is shown that, in the case of one-time magnetic field actuation, the inverse effect value is –0.25 K at a magnetostructural transition temperature TS. The second and following on/off cycles lead to a decrease in the effect by an order of magnitude to –0.03 K. Such a behavior is associated with the effect of kinetic relaxation in the martensite phase and phase transition irreversibility in the used magnetic fields. Near TC, the stable and direct effect ∆Tad = 0.23 K without degradation signs is observed.

The Physics of Metals and MetallographyVol. 125(14)
Institute of Physics. HI Amirkhanova (RU), Vietnam Academy of Science and Technology (VN)
Openalex Percentile: Top 42%
Shape Memory Alloy Transformations
0.35
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