4.7 Article

Controlled synthesis of various SrTiO3 morphologies and their effects on photoelectrochemical cathodic protection performance

期刊

CERAMICS INTERNATIONAL
卷 48, 期 14, 页码 20228-20236

出版社

ELSEVIER SCI LTD
DOI: 10.1016/j.ceramint.2022.03.302

关键词

Photoelectrochemical cathodic protection; Morphology control; SrTiO 3; 304 stainless steel

资金

  1. Youth fund of Hebei Province Education Department [QN2017117]
  2. Hebei Natural Science Funds for the Joint Research of Iron and Steel [E2019209374]
  3. Hebei Natural Science Foundation iron and steel joint fund [E2021209002]

向作者/读者索取更多资源

This paper investigates the effect of micro morphology on the photoelectrochemical cathodic protection performance of SrTiO3. A series of samples with controllable morphology were prepared. The results show that the flower-like microspheres (FLMs) samples exhibit better photochemical performance, with higher photocurrent density and larger negative shift in open circuit potential.
As an n-type semiconductor with typical perovskite structure, SrTiO3 has broad research prospects in photochemical cathodic protection because of its suitable energy band structure. However, there is a lack of research on the effect of SrTiO3 micro morphology on Photoelectrochemical cathodic protection performance. In this paper, a series of SrTiO3 samples with controllable morphology were designed and prepared by changing the ratio of alcohol to water in the solvent, including nanoparticles (NPs), nano ball (NBs), nano rod (NRs), coral stone-like microspheres (CSLMs) and flower-like microspheres (FLMs). The experimental results show that FLMs samples have better photochemical cathodic protection performance. Under the condition of on light, the photocurrent density of FLMs samples reaches 9.2 mu A. The photocurrent density of NPs samples is only 2.5 mu A. The former is about 3.6 times that of the latter. The open circuit potential of FLMs samples has shifted from -0.18 V to -0.42 V, with a negative shift of 240 mV, while CSLMs samples have only a negative shift of 180 mV. In contrast, FLMs samples have a more negative shift of 60 mV. After four light cycle experiments, the performance of FLMs samples is stable without obvious change.

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