| People | Locations | Statistics |
|---|---|---|
| Naji, M. |
| |
| Motta, Antonella |
| |
| Aletan, Dirar |
| |
| Mohamed, Tarek |
| |
| Ertürk, Emre |
| |
| Taccardi, Nicola |
| |
| Kononenko, Denys |
| |
| Petrov, R. H. | Madrid |
|
| Alshaaer, Mazen | Brussels |
|
| Bih, L. |
| |
| Casati, R. |
| |
| Muller, Hermance |
| |
| Kočí, Jan | Prague |
|
| Šuljagić, Marija |
| |
| Kalteremidou, Kalliopi-Artemi | Brussels |
|
| Azam, Siraj |
| |
| Ospanova, Alyiya |
| |
| Blanpain, Bart |
| |
| Ali, M. A. |
| |
| Popa, V. |
| |
| Rančić, M. |
| |
| Ollier, Nadège |
| |
| Azevedo, Nuno Monteiro |
| |
| Landes, Michael |
| |
| Rignanese, Gian-Marco |
|
Emre, Baris
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (6/6 displayed)
- 2024Revealing contrary contributions of the magnetic and lattice entropy to the inverse magnetocaloric effect in magnetic shape memory alloycitations
- 2024Tuning of the magneto-caloric effects in Ni<sub>43</sub>Mn<sub>46</sub>In<sub>11</sub> magnetic shape memory alloys by substitution of boroncitations
- 2024Tuning of the magneto-caloric effects in Ni 43 Mn 46 In 11 magnetic shape memory alloys by substitution of boroncitations
- 2023Investigation of the inverse magnetocaloric effect with the fraction methodcitations
- 2022Investigation of the complex magnetic behavior of Ni 46.86 Co 2.91 Mn 38.17 Sn 12.06 (at%) magnetic shape memory alloy at low temperaturescitations
- 2019Investigation of Ti substituting for Ni on magnetic, magnetocaloric and phase transition characteristics of Ni 50 Mn 36 In 14citations
Places of action
| Organizations | Location | People |
|---|
article
Investigation of the inverse magnetocaloric effect with the fraction method
Abstract
<jats:title>Abstract</jats:title><jats:p>In this study, we examine Ni<jats:sub>49</jats:sub>Nb<jats:sub>1</jats:sub>Mn<jats:sub>36</jats:sub>In<jats:sub>14</jats:sub> (nom. at.%) magnetic shape memory alloy (MSMA) to illustrate the inverse magnetocaloric effect (MCE) using the fraction method. The magnetic entropy change, <jats:inline-formula><jats:tex-math><?CDATA $ {S_{{{mag}}}}$?></jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"><mml:mi mathvariant="normal">Δ</mml:mi><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mrow><mml:mtext>mag</mml:mtext></mml:mrow></mml:mrow></mml:msub></mml:mrow></mml:math><jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="cmacd3ceieqn1.gif" xlink:type="simple" /></jats:inline-formula>, was calculated with both, the fraction method and the thermomagnetic Maxwell relation. Our results demonstrate that there exists a large magnetization difference between field-cooling and field-heating histories in Ni<jats:sub>49</jats:sub>Nb<jats:sub>1</jats:sub>Mn<jats:sub>36</jats:sub>In<jats:sub>14</jats:sub> (nom. at.%) MSMA, which can be attributed to the pinning of lattice entropy and magnetic entropy, as it is well-known that the temperature and applied magnetic fields have an opposing effect on the total entropy change. In addition, we describe the inverse MCE and the contradictory roles on the total entropy change between the two stimuli via the fraction method.</jats:p>