Aswathappa Sivakumar, Dai Lidong, Jude Dhas S Sahaya, Dhas S A Martin Britto, Laha Sourav, Kumar Raju Suresh, Almansour Abdulrahman I
Key Laboratory of High-Temperature and High-Pressure Study of the Earth's Interior, Institute of Geochemistry, Chinese Academy of Sciences, Guiyang, Guizhou 550081, China.
Department of Physics, Kings Engineering College, Sriperumbudur, Chennai, Tamilnadu 602117, India.
Inorg Chem. 2024 Jan 8;63(1):576-592. doi: 10.1021/acs.inorgchem.3c03461. Epub 2023 Dec 18.
Herein, we describe the solid-state fusion of rod-shaped to honeycomb-shaped cadmium oxide particles (CdO NPs) caused by the process of repeated exposure to acoustic shock waves. Significant changes have been observed in structurally and morphologically dependent properties. For instance, at the 200-shocked condition, the high-pressure CdO-B2 phase is present as a secondary phase wherein all of the rod-shaped particles have been transformed into honeycomb-shaped CdO particles which possess comparatively higher specific-capacitance than CdO nanorods (NRs). The computed specific capacitance values for the 0, 100, and 200 shocked samples at a scan rate of 100 m V s are computed to be 433, 415, and 583 F g, respectively. The second-stage decomposition temperature points of the CdO NPs have significantly increased in accordance with the morphological changes from rod to honeycomb patterns such that the values are 343, 526, and 534 °C, respectively, for 0, 100, and 200 shocked conditions. Note that such honeycomb nanostructured CdO particles by shock-wave processing have never been observed, to date. Due to the superior energy storage abilities as well as the spectacular high thermal stability of the honeycomb CdO nanostructures compared to CdO NRs, shocked CdO with honeycomb nanostructures can be considered as energy storage materials.
在此,我们描述了由于反复暴露于声冲击波过程而导致的棒状氧化镉颗粒(CdO NPs)向蜂窝状氧化镉颗粒的固态融合。在结构和形态相关性质方面已观察到显著变化。例如,在200次冲击条件下,高压CdO - B2相作为第二相存在,其中所有棒状颗粒均已转变为蜂窝状CdO颗粒,其比电容比CdO纳米棒(NRs)相对更高。在扫描速率为100 mV s时,计算得出的0次、100次和200次冲击样品的比电容值分别为433、415和583 F g。随着从棒状到蜂窝状形态的变化,CdO NPs的第二阶段分解温度点显著升高,对于0次、100次和200次冲击条件,其值分别为343、526和534 °C。请注意,迄今为止从未观察到通过冲击波处理得到的这种蜂窝状纳米结构CdO颗粒。由于与CdO NRs相比,蜂窝状CdO纳米结构具有卓越的能量存储能力以及惊人的高热稳定性,具有蜂窝状纳米结构的冲击CdO可被视为能量存储材料。