• Journal of Inorganic Materials
  • Vol. 35, Issue 6, 633 (2020)
Ying YU1, Hongliang DU1、2、*, Zetian YANG1, Li JIN2, and Shaobo QU1
Author Affiliations
  • 1Department of Basic Sciences, Air Force Engineering University, Xi'an 710051, China
  • 2Electronic Materials Research Laboratory, School of Electronic and Information Engineering, Xi’an Jiaotong University, Xi’an 710049, China
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    DOI: 10.15541/jim20190308 Cite this Article
    Ying YU, Hongliang DU, Zetian YANG, Li JIN, Shaobo QU. Electrocaloric Effect of Lead-free Bulk Ceramics: Current Status and Challenges[J]. Journal of Inorganic Materials, 2020, 35(6): 633 Copy Citation Text show less

    Abstract

    Solid-state cooling technology based on the electrocaloric (EC) effect is attracting increasing attention as an important alternative for traditional cooling systems because of its advantages of high efficiency, environmental friendliness, light weight, low cost, and easy miniaturization. Ferroelectric materials are suitable candidates for EC refrigeration due to their large polarization and entropy change through applying or removing an external electric field. Recently, study on the EC effect of lead-free bulk ceramics has become one of hot topics on ferroelectric community due to the requirements of sustainable development. In this review, we firstly introduce the significant history events in EC research and the basic principles of EC refrigeration. Then, design strategy for achieving a large EC temperature change near room temperature and a wide using range is summarized. Subsequently, we systematically review the research status of EC effect in BaTiO3-based, Bi0.5Na0.5TiO3-based and K0.5Na0.5NbO3-based lead-free bulk ceramics and discuss their advantages as well as challenges. Finally, we propose some prospects for the future work on EC effect in lead-free bulk ceramics.
    Ying YU, Hongliang DU, Zetian YANG, Li JIN, Shaobo QU. Electrocaloric Effect of Lead-free Bulk Ceramics: Current Status and Challenges[J]. Journal of Inorganic Materials, 2020, 35(6): 633
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