Kim Jin-Sol, Kim Il-Ho
Department of Materials Science and Engineering, College of Engineering, Korea National University of Transportation, Chungju 27469, Republic of Korea.
Materials (Basel). 2024 Nov 11;17(22):5497. doi: 10.3390/ma17225497.
The optimal conditions for synthesizing a pure chalcopyrite CuFeS phase were thoroughly investigated through the combination of mechanical alloying (MA) and hot pressing (HP) processes. The MA process was performed at a rotational speed of 350 rpm for durations ranging from 6 to 24 h under an Ar atmosphere, ensuring proper mixing and alloying of the starting materials. Afterward, MA-synthesized chalcopyrite powder was subjected to HP at temperatures between 723 K and 823 K under a pressure of 70 MPa for 2 h in a vacuum. This approach aimed to achieve phase consolidation and densification. A thermal analysis via differential scanning calorimetry (DSC) revealed distinct endothermic peaks at the range of 740-749 K and 1169-1170 K, corresponding to the synthesis of the chalcopyrite phase and its melting point, respectively. An X-ray diffraction (XRD) analysis confirmed the successful synthesis of the tetragonal chalcopyrite phase across all samples. However, a minor secondary phase, identified as CuFeS (talnakhite), was observed in the sample hot-pressed at the highest temperature of 823 K. This secondary phase could result from slight compositional deviations or local phase transformations at elevated temperatures. The thermoelectric properties of the CuFeS samples were evaluated as a function of the HP temperatures. As the HP temperature increased, the electrical conductivity exhibited a corresponding rise, likely due to enhanced densification and reduced grain boundary resistance. However, this increase in electrical conductivity was accompanied by a decrease in both the Seebeck coefficient and thermal conductivity. The reduction in the Seebeck coefficient could be attributed to the higher carrier concentration resulting from improved electrical conductivity, while the decrease in thermal conductivity was likely due to reduced phonon scattering facilitated by the grain boundaries. Among the samples, the one that was hot-pressed at 773 K displayed the most favorable thermoelectric performance. It achieved the highest power factor of 0.81 mWmK at 523 K, indicating a good balance between the Seebeck coefficient and electrical conductivity. Additionally, this sample achieved a maximum figure-of-merit (ZT) of 0.32 at 723 K, a notable value for chalcopyrite-based thermoelectric materials, indicating its potential for mid-range temperature applications.
通过机械合金化(MA)和热压(HP)工艺相结合的方法,对合成纯黄铜矿CuFeS相的最佳条件进行了深入研究。机械合金化过程在氩气气氛下,以350 rpm的转速进行6至24小时,确保起始材料充分混合和合金化。之后,将机械合金化合成的黄铜矿粉末在真空中于723 K至823 K的温度、70 MPa的压力下进行2小时的热压。此方法旨在实现相固结和致密化。通过差示扫描量热法(DSC)进行的热分析显示,在740 - 749 K和1169 - 1170 K范围内有明显的吸热峰,分别对应黄铜矿相的合成及其熔点。X射线衍射(XRD)分析证实所有样品均成功合成了四方黄铜矿相。然而,在823 K最高温度下热压的样品中观察到少量次生相,鉴定为CuFeS(塔尔纳赫矿)。该次生相可能是由于高温下轻微的成分偏差或局部相变导致的。对CuFeS样品的热电性能作为热压温度的函数进行了评估。随着热压温度升高,电导率相应增加,这可能是由于致密化增强和晶界电阻降低所致。然而,电导率的这种增加伴随着塞贝克系数和热导率的降低。塞贝克系数的降低可归因于电导率提高导致载流子浓度增加,而热导率的降低可能是由于晶界促进的声子散射减少所致。在所有样品中,在773 K下热压的样品表现出最优异的热电性能。它在523 K时实现了0.81 mWmK的最高功率因子,表明塞贝克系数和电导率之间达到了良好的平衡。此外,该样品在723 K时实现了0.32的最大优值(ZT),对于基于黄铜矿的热电材料来说是一个显著的值,表明其在中温应用方面的潜力。