Extremely relative cooling power of Cu0.35Zn0.65Fe2O4

2021 ◽  
Vol 394 ◽  
pp. 127204
Author(s):  
Mahmoud A. Hamad ◽  
O.M. Hemeda ◽  
Hatem R. Alamri ◽  
Ashraf M. Mohamed
2011 ◽  
Author(s):  
S. Shanmukharao Samatham ◽  
D. Venkateshwarlu ◽  
Swati Pandya ◽  
Mohan Gangrade ◽  
L. S. Sharath Chandra ◽  
...  

RSC Advances ◽  
2020 ◽  
Vol 10 (35) ◽  
pp. 20646-20653 ◽  
Author(s):  
Yun Zhang ◽  
Xiaojie Xu

Experimental vs. predicted relative cooling power of lanthanum manganites.


RSC Advances ◽  
2016 ◽  
Vol 6 (81) ◽  
pp. 77284-77290 ◽  
Author(s):  
Abd El-Moez A. Mohamed ◽  
Mohamed A. Mohamed ◽  
V. Vega ◽  
B. Hernando ◽  
A. M. Ahmed

The effect of interface size on the relative cooling power and magnetoresistive properties of La0.7Ba0.3MnO3 compounds is investigated.


2011 ◽  
Vol 23 (5) ◽  
pp. 052201 ◽  
Author(s):  
Q Zhang ◽  
S Thota ◽  
F Guillou ◽  
P Padhan ◽  
V Hardy ◽  
...  

2009 ◽  
Vol 154 ◽  
pp. 163-168 ◽  
Author(s):  
R.A. Szymczak ◽  
Aleksandra Kolano-Burian ◽  
Roman Kolano ◽  
R. Puzniak ◽  
V.P. Dyakonov ◽  
...  

The magnetocaloric effect in La0.6Ca0.4MnO3 manganite has been investigated. The isothermal magnetization versus applied magnetic field at various temperatures in the vicinity of Curie temperature was measured, and the temperature dependence of magnetic entropy change was determined using Maxwell’s relation. This value is comparable to that in Gd. Nevertheless, the relative cooling power of La0.6Ca0.4MnO3 was shown to be considerably lower than that of Gd. The experimental results have been analyzed in frames of a phenomenological statistical model. This model considers explicitly Jahn-Teller interactions and allows prediction of the field dependences of the magnetic entropy change and the relative cooling power.


Materials ◽  
2019 ◽  
Vol 12 (2) ◽  
pp. 309 ◽  
Author(s):  
María Botello-Zubiate ◽  
María Grijalva-Castillo ◽  
Daniel Soto-Parra ◽  
Renee Sáenz-Hernández ◽  
Carlos Santillán-Rodríguez ◽  
...  

Manganites of the family La0.7Ca0.3−xSrxMnO3 were fabricated by four preparation methods: (a) the microwave-assisted sol-gel Pechini method; (b) sol-gel Pechini chemical synthesis; (c) solid-state reaction with a planetary mill; and (d) solid-state reaction with an attritor mill, in order to study the effect of the preparation route used on its magnetocaloric and magnetic properties. In addition, the manganites manufactured by the Pechini sol-gel method were compacted using Spark Plasma Sintering (SPS) to determine how the consolidation process influences its magnetocaloric properties. The Curie temperatures of manganites prepared by the different methods were determined in ~295 K, with the exception of those prepared by a solid-state reaction with an attritor mill which was 301 K, so there is no correlation between the particle size and the Curie temperature. All samples gave a positive slope in the Arrot plots, which implies that the samples underwent a second order Ferromagnetic (FM)–Paramagnetic (PM) phase transition. Pechini sol-gel manganite presents higher values of Relative Cooling Power (RCP) than the solid-state reaction manganite, because its entropy change curves are smaller, but wider, associated to the particle size obtained by the preparation method. The SPS technique proved to be easier and faster in producing consolidated solids for applications in active magnetic regenerative refrigeration compared with other compaction methods.


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