journal article·2023-08-11

Multiferroic Electroactive Polymer Blend/Ferrite Nanocomposite Flexible Films for Cooling Devices

Prabhakaran Thandapani, Radhamanohar Aepuru, Fanny Béron, Mangalaraja Ramalinga Viswanathan, Kokkarachedu Varaprasad, Fabio Luis Zabotto, José A. Jiménez, Juliano C. Denardin

ACS Applied Polymer Materials· Volume 5· Issue 8
Publisher page

Abstract

In recent days, the interest toward the development of multicaloric materials for cooling application is increasing, whereas multiferroic materials would be the suitable alternative to the conventional refrigerants. To explore them, the poly(methyl methacrylate)/poly(vinylidenefluoride- co -hexafluoropropylene) (PMMA/PVDF-HFP) blend and PMMA/PVDF-HFP/Zn 0.5 Cu 0.5 Fe 2 O 4 flexible multiferroic nanocomposite films were fabricated by the solution casting method. The structural analyses prove that the strong interfacial interaction between the PMMA/PVDF-HFP blend and the Zn 0.5 Cu 0.5 Fe 2 O 4 (ZCF) through hydroxyl (−OH) and carbonyl group bonding with PVDF-HFP enhanced the thermal stability and suppressed the electroactive β phase from 67 to 62%. Experimental results show that 10 wt % of superparamagnetic ZCF nanoparticles with a particle size of 6.8 nm induced both the magnetocaloric and magnetoelectric effects in a nonmagnetic PMMA/PVDF-HFP ferroelectric matrix at room temperature. A set of isothermal magnetization curves were recorded in the magnetic field strength of 0–40 kOe and a temperature range of 2–400 K. The maximum magnetic entropy changes (Δ S M ) of −0.69 J·kg –1 K –1 of ZCF nanoparticles and −0.094 J·kg –1 K –1 of PMMA/PVDF-HFP/ZCF nanocomposites showed an interesting table-like flat variation in the temperature range of 100–400 K as a function of the magnetic field. The samples display a large temperature span with a relative cooling power of 293 and 40 J·kg –1 for ZCF and PMMA/PVDF-HFP/ZCF, respectively. The magnetoelectric effect of the PMMA/PVDF-HFP/ZCF composite was proved, but it generated only 1.42 mV/m·Oe in the applied field of 5 kOe. Hence, the entropy change of the present nanocomposite was only due to the magnetocaloric effect, where the magnetoelectric cross-coupling coefficient was negligible. The multicaloric effect could be established if the nanocomposite showed a larger magnetoelectric cross-coupling in addition to the magnetocaloric effect. This approach provides the research findings in functional multiferroic polymer nanocomposites for miniaturized cooling devices.
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Research context

OpenAlex topics: Multiferroics and related materials · Ferroelectric and Piezoelectric Materials · Vibration Control and Rheological Fluids

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Physics, School of Advanced Sciences (SAS), VIT-AP University, Amaravati 522237 Andhra Pradesh, India

Departamento de Ingeniería Mecánica, Facultad de Ciencias Fisicas y Matematicas, Universidad de Chile, Beauchef 851, Santiago 8370456, Chile

Materials and Low-temperature Laboratory (LMBT), Institute of Physics “Gleb Wataghin”(IFGW), University of Campinas (UNICAMP), Campinas 13083-859, São Paulo, Brazil

Faculty of Engineering and Science, Universidad Adolfo Ibáñez, Diagonal las Torres, 2640 Peñalolén, Santiago, Chile

Facultad de Ingeniería, Arquitectura y Diseño, Universidad San Sebastián, Lientur 1457, Concepción 00043, Chile

Physics Department, Federal University of São Carlos, SP CEP, São Carlos 13565-905, Brazil

Department of Physical Metallurgy, CENIM-CSIC, Madrid 28040, Spain

Center for the Development of Nanoscience and Nanotechnology (CEDENNA), Physics Department, University of Santiago of Chile (USACH), Santiago 7190006, Chile

Funding

Funda??o de Amparo ? Pesquisa do Estado de S?o Paulo · Fondo Nacional de Desarrollo Cient?fico y Tecnol?gico

References (59)

Show source-provided references
1. 10.1126/science.abb097310.1126/science.abb0973 ↗
2. 10.1016/j.enconman.2018.10.02510.1016/j.enconman.2018.10.025 ↗
3. 10.1016/j.ijrefrig.2016.04.02010.1016/j.ijrefrig.2016.04.020 ↗
4. 10.1038/srep2662910.1038/srep26629 ↗
5. 10.1016/j.ssc.2012.08.01610.1016/j.ssc.2012.08.016 ↗
6. 10.1103/PhysRevLett.124.16720110.1103/PhysRevLett.124.167201 ↗
7. 10.1126/science.aan598010.1126/science.aan5980 ↗
8. 10.1039/D0TA04465B10.1039/D0TA04465B ↗
9. 10.1126/science.115965510.1126/science.1159655 ↗
10. 10.1002/adma.20180194910.1002/adma.201801949 ↗
11. 10.1063/5.013888710.1063/5.0138887 ↗
12. 10.1021/acsnano.5b0337110.1021/acsnano.5b03371 ↗
13. 10.1063/1.186232310.1063/1.1862323 ↗
14. 10.1039/C3RA47462C10.1039/C3RA47462C ↗
15. 10.1049/iet-nde.2017.000710.1049/iet-nde.2017.0007 ↗
16. 10.1016/j.ssi.2015.09.01710.1016/j.ssi.2015.09.017 ↗
17. 10.1002/pssa.20170084210.1002/pssa.201700842 ↗
18. 10.1021/acs.jpcc.9b0707610.1021/acs.jpcc.9b07076 ↗
19. 10.1016/j.powtec.2015.03.02210.1016/j.powtec.2015.03.022 ↗
20. 10.1016/j.jmmm.2014.04.07010.1016/j.jmmm.2014.04.070 ↗
21. 10.1039/C8NR02368A10.1039/C8NR02368A ↗
22. 10.1016/j.mtchem.2021.10051110.1016/j.mtchem.2021.100511 ↗
23. 10.1002/aelm.20180003010.1002/aelm.201800030 ↗
24. 10.1016/j.matchemphys.2012.09.06410.1016/j.matchemphys.2012.09.064 ↗
25. 10.1016/j.mseb.2017.09.02410.1016/j.mseb.2017.09.024 ↗
26. 10.1039/C4TC02183E10.1039/C4TC02183E ↗
27. 10.1039/c6ra18032a10.1039/c6ra18032a ↗
28. 10.1038/s41598-019-54635-810.1038/s41598-019-54635-8 ↗
29. 10.1016/j.jmmm.2020.16688410.1016/j.jmmm.2020.166884 ↗
30. 10.1016/j.matdes.2019.10839910.1016/j.matdes.2019.108399 ↗
31. 10.22226/2410-3535-2021-2-213-21710.22226/2410-3535-2021-2-213-217 ↗
32. 10.1016/j.jallcom.2020.15681910.1016/j.jallcom.2020.156819 ↗
33. 10.1063/1.356044510.1063/1.3560445 ↗
34. 10.1063/1.514071010.1063/1.5140710 ↗
35. 10.1007/s10853-005-2182-610.1007/s10853-005-2182-6 ↗
36. 10.1088/1755-1315/108/4/04209710.1088/1755-1315/108/4/042097 ↗
37. 10.1016/j.matdes.2019.10835410.1016/j.matdes.2019.108354 ↗
38. 10.1016/j.matchemphys.2019.12221910.1016/j.matchemphys.2019.122219 ↗
39. 10.1063/1.508175810.1063/1.5081758 ↗
40. 10.1016/j.heliyon.2016.e0013410.1016/j.heliyon.2016.e00134 ↗
41. 10.1039/C3RA42244E10.1039/C3RA42244E ↗
42. 10.1039/C7RA03250A10.1039/C7RA03250A ↗
43. 10.1002/polb.1994.09032050910.1002/polb.1994.090320509 ↗
44. 10.1007/s00339-020-03698-w10.1007/s00339-020-03698-w ↗
45. 10.1007/s10965-019-1704-x10.1007/s10965-019-1704-x ↗
46. 10.1016/j.tca.2011.06.01010.1016/j.tca.2011.06.010 ↗
47. 10.1007/s10948-018-4982-310.1007/s10948-018-4982-3 ↗
48. 10.1063/1.500591310.1063/1.5005913 ↗
49. 10.1063/1.335801710.1063/1.3358017 ↗
50. 10.1016/j.jallcom.2004.03.13710.1016/j.jallcom.2004.03.137 ↗
51. 10.1166/jnn.2013.709210.1166/jnn.2013.7092 ↗
52. 10.1016/j.pmatsci.2017.10.00510.1016/j.pmatsci.2017.10.005 ↗
53. 10.1002/pssa.1970003040310.1002/pssa.19700030403 ↗
54. 10.1016/j.compositesb.2018.12.01010.1016/j.compositesb.2018.12.010 ↗
55. 10.1016/j.ceramint.2018.08.23410.1016/j.ceramint.2018.08.234 ↗
56. 10.1016/j.jallcom.2019.05.01310.1016/j.jallcom.2019.05.013 ↗
57. 10.1007/s10971-016-4296-510.1007/s10971-016-4296-5 ↗
58. 10.1007/s00339-018-2082-710.1007/s00339-018-2082-7 ↗
59. 10.1088/0022-3727/46/34/34530410.1088/0022-3727/46/34/345304 ↗