Enhancing the Elastocaloric Strength by Combining Positive and Negative Elastocaloric Effects
Solid‐state refrigeration has received widespread attention recently because of its high refrigeration efficiency and environmental protection. Compared with other solid‐state refrigeration technologies, elastocaloric effects have great application potential. However, the current temperature change...
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Veröffentlicht in: | Physica status solidi. PSS-RRL. Rapid research letters 2022-08, Vol.16 (8), p.n/a |
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Sprache: | eng |
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Zusammenfassung: | Solid‐state refrigeration has received widespread attention recently because of its high refrigeration efficiency and environmental protection. Compared with other solid‐state refrigeration technologies, elastocaloric effects have great application potential. However, the current temperature change of elastocaloric effects is still low. This work explores the change law of phase transition temperature of ferroelectric materials by applying the external stress based on the thermodynamic calculation. It can be found that ferroelectric materials’ positive and negative elastocaloric effects can peak at the same temperature, so here a device to combine the positive and negative elastocaloric effects of Ba0.7Sr0.3TiO3 and BaZr0.015Ti0.085O3 is designed. This device can achieve a ΔT of 3.18 K near room temperature under applied stress of 200 MPa, which is twice as large as that of 1.4 K in BCZTO‐Fe under the same stress condition. And it can be raised to 4.1 K after applying an electric field of 10 MV m−1. It is the first time to combine positive and negative elastocaloric effects to achieve high cooling near room temperature, which provides a new solution for efficient cooling near room temperature.
A device to combine the positive and negative elastocaloric effects of Ba0.7Sr0.3TiO3 and BaZr0.015Ti0.085O3 is designed. This device can achieve a ΔT of 3.18 K near room temperature under applied stress of 200 MPa and it can be raised to 4.1 K after applying an electric field of 10 MV m−1. |
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ISSN: | 1862-6254 1862-6270 |
DOI: | 10.1002/pssr.202200183 |