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首页> 外文期刊>Journal of Electronic Materials >Synthesis and Thermoelectric Properties of Zr(x)Ti(1-x)NiSn(0.98)Sb(0.02)n-Type Half-Heusler Materials
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Synthesis and Thermoelectric Properties of Zr(x)Ti(1-x)NiSn(0.98)Sb(0.02)n-Type Half-Heusler Materials

机译:Zr(X)Ti(1-X)NISN(0.02)的合成和热电性能(0.02)N型半风素材料

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Hf-free ZrxTi1-xNiSn0.98Sb0.02 (x = 0.25, 0.5, 0.75) n-type half-Heusler (HH) thermoelectric materials were synthesized by a serial processing method including induction melting (IM), annealing, ball milling, and spark plasma sintering (SPS). For comparison, a Hf-containing half-Heusler Hf0.25Zr0.25Ti0.5NiSn0.98Sb0.02 ingot was also alloyed by arc melting, and the effects of Hf on the thermoelectric properties were estimated. The ZrxTi1-xNiSn0.98Sb0.02 HH materials were nearly pure according to the x-ray diffraction analysis, but microscopic investigation revealed impurity phase inclusions of unalloyed Sn, Zr, and Ti. The power factor (PF) of the Hf-free HH materials reached the maximum value of 4.31 mWm(-1) K-2 at 823 K in Zr0.75Ti0.25NiSn0.98Sb0.02, which was higher than Hf0.25Zr0.25Ti0.5NiSn0.98Sb0.02 (4.01 mWm(-1) K-2 at 773 K) in this study. However, the thermal conductivity of the Hf-free samples was significantly higher, by which the maximum dimensionless figure of merit was slightly lower (ZT(max) = 0.92 in Zr0.75Ti0.25NiSn0.98Sb0.02 at 873 K) than that of Hf0.25Zr0.25Ti0.5NiSn0.98Sb0.02 (ZT(max) = 1.03 at 873 K). The thermal conductivity was decomposed into lattice and electronic contributions, and the possible correlation with Ni off-stoichiometry is discussed.
机译:无Hf ZrxTi1-xNiSn0。98Sb0。采用感应熔炼(IM)、退火、球磨和放电等离子烧结(SPS)等一系列工艺方法合成了02(x=0.25,0.5,0.75)n型半赫勒(HH)热电材料。相比之下,含有半个Heusler Hf0的Hf。25Zr0。25Ti0。5NiSn0。98Sb0。02铸锭也通过电弧熔炼进行合金化,并评估了Hf对热电性能的影响。ZrxTi1-xNiSn0。98Sb0。根据x射线衍射分析,02 HH材料几乎是纯的,但微观调查显示,杂质相夹杂物为非合金Sn、Zr和Ti。无Hf HH材料的功率因数(PF)在Zr0中823K时达到最大值4.31MWm(-1)K-2。75Ti0。25NiSn0。98Sb0。02,高于Hf0。25Zr0。25Ti0。5NiSn0。98Sb0。02(773K时为4.01MWm(-1)K-2)。然而,无Hf样品的热导率显著较高,最大无量纲优值略低(ZT(max)=0.92 in Zr0)。75Ti0。25NiSn0。98Sb0。在873K时为0.02),高于Hf0。25Zr0。25Ti0。5NiSn0。98Sb0。02(ZT(最大值)=873 K时为1.03)。将热导率分解为晶格贡献和电子贡献,并讨论了与化学计量比无关的可能关联。

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