无机材料学报 ›› 2021, Vol. 36 ›› Issue (4): 347-354.DOI: 10.15541/jim20200417 CSTR: 32189.14.10.15541/jim20200417
所属专题: 能源材料论文精选(2021); 【虚拟专辑】热电材料(2020~2021)
杨青雨1,2(), 仇鹏飞1,2, 史迅1,2(
), 陈立东1,2
收稿日期:
2020-07-27
修回日期:
2020-09-14
出版日期:
2021-04-20
网络出版日期:
2020-09-20
通讯作者:
史 迅, 研究员. E-mail: xshi@mail.sic.ac.cn
作者简介:
杨青雨(1995-), 男, 博士研究生. E-mail: yangqingyu@student.sic.ac.cn
基金资助:
YANG Qingyu1,2(), QIU Pengfei1,2, SHI Xun1,2(
), CHEN Lidong1,2
Received:
2020-07-27
Revised:
2020-09-14
Published:
2021-04-20
Online:
2020-09-20
Contact:
SHI Xun, professor. E-mail: xshi@mail.sic.ac.cn
About author:
YANG Qingyu(1995-), male, PhD candidate. E-mail: yangqingyu@student.sic.ac.cn
Supported by:
摘要:
作为高熵合金设计思想的延伸, 熵工程可从电子和声子输运两方面引导热电材料的性能优化, 在多种热电材料体系已经获得了成功应用。特别是, 熵具有内禀的类似基因特性, 可以作为热电材料的指征因子, 对多元热电材料实现快速筛选。本文首先揭示熵作为热电材料基因特性的内禀原因, 阐述构型熵增加导致材料晶体结构对称性增强、泽贝克系数提升、晶格热导率下降的物理机制; 然后着重介绍熵工程在类液态材料和IV-VI族半导体等典型热电材料体系中的应用, 总结熵工程提高材料热电性能的研究进展; 并介绍多元单相高熵热电材料的热力学稳定性预测方法; 最后指出了熵工程将来的研究重点。
中图分类号:
杨青雨, 仇鹏飞, 史迅, 陈立东. 熵工程在热电材料中的应用[J]. 无机材料学报, 2021, 36(4): 347-354.
YANG Qingyu, QIU Pengfei, SHI Xun, CHEN Lidong. Application of Entropy Engineering in Thermoelectrics[J]. Journal of Inorganic Materials, 2021, 36(4): 347-354.
图2 Cu2(S/Se/Te)体系泽贝克系数与构型熵的关系[10]
Fig. 2 Room-temperature Seebeck coefficient as a function of configurational entropy in Cu2(S/Se/Te)-based multicomponent materials[10]
图3 代表性热电材料晶格热导率与构型熵的关系[10,39-40]
Fig. 3 Lattice thermal conductivity as a function of configurational entropy for typical TE materials[10,39-40] The red zone presents the minimum lattice thermal conductivity
图5 Cu2X (X=S, Te, Se)体系泽贝克系数与载流子浓度的关系[10]
Fig. 5 Carrier concentration dependence of room-temperature Seebeck coefficient in Cu2(S/Se/Te)-based TE materials with different crystal symmetry[10]
图6 (Sn, Ge, Pb, Mn)Te体系(a)泽贝克系数和(b)晶格热导率与构型熵的关系[39]
Fig. 6 (a) Seebeck coefficient and (b) lattice thermal conductivity as a function of configurational entropy in (Sn, Ge, Pb, Mn)Te-based materials[39]
图7 固溶吉布斯自由能与平均溶解度参数$\bar{\delta }$和材料组元数n的关系[10] (1 ? = 0.1 nm)
Fig. 7 Gibbs free energy as a function of the average solubility parameter$(\bar{\delta })$for given multicomponent TE materials with different number of components[10] (1 ? = 0.1 nm)
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