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中国物理学会期刊

熔融旋甩制备Co掺杂TiNiCoxSn合金的热电性能

CSTR: 32037.14.aps.73.20240112

Thermoelectric properties of Co doped TiNiCoxSn alloys fabricated by melt spinning

CSTR: 32037.14.aps.73.20240112
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  • TiNiSn基 half-Heusler高温热电材料具有较高的功率因子, 但其也具有较高的晶格热导率, 这极大地阻碍了其热电性能的提升. 本文采用熔融旋甩快淬与放电等离子烧结工艺制备TiNiCoxSn (x = 0—0.05)样品, 研究磁性Co元素掺杂对材料的相组成、微观结构和热电性能. 结果表明, 该制备工艺能够直接获得纳米晶的TiNiCoxSn样品. 在纳米晶影响下的样品的热导率明显低于块体材料的热导率, 平均降幅约为17.8%. 在Co掺杂后样品的晶粒尺寸进一步降低, 与TiNiSn基体相比, TiNiCoxSn样品的热导率显著降低, 最大降幅约为38.9%, 其中晶格热导率最低值为3.19 W/(m·K), 最大降幅约为42.6%. 随着Co掺杂量x的增大TiNiCoxSn样品出现n/p转变, 电导率随x增大而逐渐下降, 电输运性能劣化, 功率因子缓慢减小, 其中TiNiSn样品在700 K时获得29.56 W/(m·K2)的最高功率因子. ZT值随Co掺杂量x的增大而逐渐降低, TiNiSn样品在900 K时的最大ZT值为0.48. 本工作表明采用熔融旋甩制备工艺及磁性Co掺杂能够有效降低TiNiSn材料的热导率.

     

    Although TiNiSn-based half-Heusler thermoelectric materials obtain high power factors, their high lattice thermal conductivity greatly hinders the improvement of thermoelectric properties. In this work, TiNiCoxSn (x = 0–0.05) samples are prepared by melt spinning combined with spark plasma sintering method, and their phase, microstructure and thermoelectric properties are studied. The XRD results show that the main phase of all samples is TiNiSn phase, and no any other impurity phases are found, indicating that the high purity single phase can be prepared by rapid quenching process combined with SPS process. In the solidification process, the large cooling rate (105–106 K/s) is conducive to obtaining the uniform nanocrystalline structure. The grains are closely packed, with grain sizes in a range of 200–600 nm. The grain sizes decrease to 50–400 nm for the Co-doping samples, which indicates that Co doping can reduce the grain size. For the x = 0 sample, the thermal conductivity of the rapid quenching sample is significantly lower than that of bulk sample, with an average decrease of about 17.8%. Compared with the TiNiSn matrix, the Co-doping sample has the thermal conductivity that decreases significantly, and the maximum decrease can reach about 38.9%. The minimum value of lattice thermal conductivity of TiNiCoxSn samples is 3.19 W/(m·K). Therefore, Co doping can significantly reduce the κl values of TiNiCoxSn (x = 0.01–0.05) samples. With the increase of Co doping amount x, n/p transition is observed in the TiNiCoxSn samples, resulting in gradually reducing the conductivity and the power factor, and finally deteriorating the electrical transport performance, of which, the TiNiSn sample obtains the highest power factor of 29.56 W/(m·K2) at 700 K. The ZT value decreases with the Co doping amount x increasing, and the maximum ZT value of TiNiSn sample at 900 K is 0.48. This work shows that the thermal conductivity of TiNiSn can be effectively reduced by using the melt spinning process and magnetic Co doping.

     

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