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Absence of Nanostructuring in NaPb_mSbTe_(m+2): Solid Solutions with High Thermoelectric Performance in the Intermediate Temperature Regime

机译:NaPb_mSbTe_(m + 2)中没有纳米结构:在中等温度下具有高热电性能的固溶体

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摘要

Thermoelectric devices directly convert heat into electrical energy and are highly desired for emerging applications in waste heat recovery. Currently, PbTe based compounds are the leading thermoelectric materials in the intermediate temperature regime (∼800 K); however, integration into commercial devices has been limited. This is largely because the performance of PbTe, which is maximized ∼900 K, is too low over the temperatures of interest for most potential commercial applications (generally under 600 K). Improving the low temperature performance of PbTe based materials is therefore critical to achieve usage outside of existing niche applications. Here, we provide an in-depth study of the cubic NaPb_(m )SbTe_(m +2) system of compounds (m = 1–20) and report that it is an excellent class of low- to medium-temperature thermoelectrics when m = 10–20. We show that the as-cast polycrystalline ingots exhibit degenerate p-type conduction and high maximum ZT s of 1.2–1.4 at 650 K when m = 6–20. Because the ingots are found to be extremely brittle, we utilize spark plasma sintering (SPS) to prepare more mechanically robust samples, and surprisingly, find that SPS results in an undesired change in charge transport toward n-type behavior. We show this unanticipated transition from p-type behavior as ingots to n-type after SPS is due to dissolution of secondary phases that are present in the ingots into the primary matrix during the SPS process, resulting in a transformation from an inhomogeneous state to a solid solution without any observable evidence of nanoscale precipitation. This is in sharp contrast to the seemingly similar AgPb_(m)SbTe_(m +2) (LAST) system, which is heavily nanostructured. The SPSed NaPb_(m )SbTe_(m +2) is doped p-type by tuning the cation stoichiometry, i.e., Na_(1+x )Pb_(m –x )Sb_(1–y )Te_(m +2). The optimized compounds have very low lattice thermal conductivities of 1.1–0.55 W·m~(–1)·K~(–1) over 300–650 K, which enhances the low-intermediate temperature performance and gives rise to maximum ZT values up to 1.6 at 673 K as well as an excellent ZT _(avg) of 1.1 over 323–673 K for m = 10, 20, making Na_(1+x )Pb_(m –x )Sb_(1–y )Te_(m +2) among the highest performing PbTe-based thermoelectrics under 650 K.
机译:热电装置将热量直接转换成电能,并且对于废热回收中的新兴应用非常需要。目前,基于PbTe的化合物是中温范围(约800 K)中的主要热电材料。然而,集成到商业设备中受到限制。这主要是因为对于大多数潜在的商业应用(通常在600 K以下),PbTe的最大性能(约900 K)在所关注的温度范围内过低。因此,提高PbTe基材料的低温性能对于在现有的特殊应用之外实现使用至关重要。在这里,我们对化合物( m = 1–20)的立方NaPb _( m)SbTe _( m +2)系统进行了深入研究,并报告说它是一类优秀的m = 10–20时为中低温热电元件。我们显示,当 m = 6-20时,铸态多晶锭在650 K时表现出简并的p型传导和1.2-1.4的最大最大ZT s。由于发现铸锭非常脆,我们利用火花等离子体烧结(SPS)来制备机械强度更高的样品,并且令人惊讶地发现,SPS导致电荷传输朝n型行为发生了不希望的变化。我们显示,在SPS之后,这种从晶锭的p型行为到n型的意外转变是由于在SPS过程中晶锭中存在的次生相溶解到初级基质中,导致了从不均匀状态到晶格的转变。固溶体,没有任何可观察到的纳米级沉淀迹象。这与看似相似的AgPb_(m)SbTe_(im +2)(LAST)系统形成了鲜明的对比,后者是高度纳米结构的。通过调节阳离子的化学计量,将SPSed NaPb _( m)SbTe _( m +2)掺杂为p型,即Na_(1+ x)Pb _( m – x)Sb_(1– y)Te _( m +2)。经过优化的化合物在300–650 K范围内具有极低的1.1–0.55 W·m〜(–1)·K〜(–1)晶格热导率,从而增强了低中间温度性能并产生了最大的在 m = 10,20时,ZT值在673 K时高达1.6,并且在323–673 K上具有出色的 ZT _(avg)1.1,使得Na_(1+ x)Pb_(在650 K以下性能最高的基于PbTe的热电之中, m – x)Sb_(1– y)Te _( m +2)。

著录项

  • 来源
    《Journal of the American Chemical Society》 |2018年第22期|7021-7031|共11页
  • 作者单位

    Department of Chemistry, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, United States;

    Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, United States;

    Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Chemistry, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, United States;

    Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Materials Science and Engineering, Northwestern University, Evanston, Illinois 60208, United States;

    Department of Chemistry, Northwestern University, Evanston, Illinois 60208, United States;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-18 03:07:20

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