Electrochemical applications of CdO-Co-ZnO nanocomposites, their synthesis and characterization reveal their multifunctional abilities

N. Rajkamal , K. Sambathkumar , K. Parasuraman , K. Bhuvaneswari , R. Uthrakumar , K. Kaviyarasu
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Abstract

In this study, we investigated the electrochemical catalysis potential of hybrid nanocomposites containing CdO, Co and ZnO nanocomposites, as opposed to Zn-O doped Co nanocomposites, have weaker Coulomb interactions due their ionic bonds. Because CdO and Co form a covalent bond, Co interacts more strongly with O than Zn. In order to reduce nanoparticle crystallinity, oxygen defects improve the interaction between −O and oxygen defects in the lattice. From SEM micrographs, it appears that CdO does not completely change under the influence of dopants. It can be seen from the SEM image that both materials have very tightly packed particles. The Co and CdO dopants in ZnO nanocomposites prevent them from absorbing a large range of visible wavelengths. It is more energy-dense for nanocomposites with 5.28 eV to compare to 5.14 eV nanocomposites. The fact that CdO matrix has a tuneable bandgap is evident since different types of dopants are used in its manufacture. There are at least three distinct absorption modes in Co nanocomposites doped with CdO, around 450, 498, and 676 cm−1. In addition to its absorption from 450 cm−1 and 498 cm−1 vibrational modes, Co-O stretching absorption along the [1 0 1] plane has also been observed at 676 cm−1. As a method of studying charge carriers, photoluminescence spectroscopy is usually used. This method can be used to analyze electron-hole pairs (e/h+) formed by semiconducting particles. It is in the blue emission range between the luminescence band of 615 nm and the valence band of 635 nm. With increasing cobalt and zinc concentrations, CdO nanomaterials lose their remanent magnetization. CdO has been demonstrated to have significant coercive effects in both pure and additively incorporated solutions regardless of their anisotropic, morphological, porosity, and particle size distribution. Electrochemical impedance spectrum measurements were conducted between 100 kHz and 0.01 Hz. According to the Nyquist plot, purity CdO, CdO doped Co, and CdO doped ZnO nanocomposites show a high frequency resistance to charge transfer. Nanocomposites that contained CdO doped Co & ZnO were exposed to UV light for 120 min to remove the solution. The degradation of MO is virtually nonexistent when no photocatalyst is present, but with a photocatalyst, degradation can reach 92.56 %.

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氧化镉-氧化钴-氧化锌纳米复合材料的电化学应用及其合成和表征揭示了其多功能能力
在本研究中,我们研究了含有 CdO、Co 和 ZnO 纳米复合材料的混合纳米复合材料的电化学催化潜能,与 Zn-O 掺杂 Co 纳米复合材料相比,Co 纳米复合材料因其离子键而具有较弱的库仑相互作用。由于 CdO 和 Co 形成共价键,Co 与 O 的相互作用比与 Zn 的相互作用更强。为了降低纳米粒子的结晶度,氧缺陷可改善晶格中 -O 与氧缺陷之间的相互作用。从扫描电镜显微照片来看,氧化镉在掺杂剂的影响下并没有完全改变。从扫描电镜图像中可以看出,两种材料的颗粒都非常紧密。ZnO 纳米复合材料中的掺杂剂 Co 和 CdO 使其无法吸收大范围的可见光波长。与 5.14 eV 纳米复合材料相比,5.28 eV 纳米复合材料的能量密度更高。由于在制造过程中使用了不同类型的掺杂剂,氧化镉基质具有可调带隙的事实显而易见。掺杂氧化镉的钴纳米复合材料至少有三种不同的吸收模式,分别在 450、498 和 676 cm-1 附近。除了 450 cm-1 和 498 cm-1 振动模式的吸收外,在 676 cm-1 处还观察到 Co-O 沿 [1 0 1] 平面的伸展吸收。作为研究电荷载体的一种方法,通常使用光致发光光谱法。这种方法可用于分析半导体粒子形成的电子-空穴对(e-/h+)。它的蓝色发射范围介于 615 纳米的发光带和 635 纳米的价带之间。随着钴和锌浓度的增加,氧化镉纳米材料会失去剩磁。事实证明,无论氧化镉的各向异性、形态、孔隙率和粒度分布如何,其在纯溶液和添加溶液中都具有显著的矫顽力效应。电化学阻抗谱测量在 100 kHz 和 0.01 Hz 之间进行。根据奈奎斯特图,纯 CdO、掺杂 CdO 的 Co 和掺杂 CdO 的 ZnO 纳米复合材料显示出高频电荷转移阻抗。将含有掺杂 CdO Co & ZnO 的纳米复合材料暴露在紫外线下 120 分钟,以去除溶液。在没有光催化剂的情况下,MO 的降解几乎不存在,但在有光催化剂的情况下,降解率可达 92.56%。
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来源期刊
Materials Science for Energy Technologies
Materials Science for Energy Technologies Materials Science-Materials Science (miscellaneous)
CiteScore
16.50
自引率
0.00%
发文量
41
审稿时长
39 days
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