Sibo Wang , Hongkui Zhang , Zhen Wen , Yue Li , Tong Zhang , Yingdong Qu , Guanglong Li
{"title":"采用C掺杂的方法优化了TiVZrNbFe高熵合金的相比和导热系数,提高了其储氢性能","authors":"Sibo Wang , Hongkui Zhang , Zhen Wen , Yue Li , Tong Zhang , Yingdong Qu , Guanglong Li","doi":"10.1016/j.materresbull.2025.113456","DOIUrl":null,"url":null,"abstract":"<div><div>High entropy alloys (HEAs) have become a new type of hydrogen storage materials due to their extensive composition adjustability and unique high entropy effect, and have important application potential. Based on <strong>TiVZrNbFe</strong> high entropy alloys doped C element, the alloy integral replacement, finally was prepared (Ti<sub>30.55</sub>V<sub>25.85</sub>Zr<sub>7.05</sub>Nb<sub>30.55</sub>Fe<sub>6.00</sub>) <sub>1-x</sub>C<sub>x</sub> (<em>x</em> = 0.01,0.03,0.05,0.07,0.09) high entropy alloys. <strong>The results show that C element promotes the formation of C14 Laves phase, and the ratio of BCC phase to C14 Laves phase increases with the increase of carbon content.</strong> In addition, the C element in Ti<sub>29.63</sub>V<sub>25.08</sub>Zr<sub>6.84</sub>Nb<sub>29.63</sub>Fe<sub>5.822</sub>C<sub>3</sub> increased the thermal conductivity and decreased the apparent activation energy of hydrogen absorption. The hydrogen absorption capacity of Ti<sub>29.63</sub>V<sub>25.08</sub>Zr<sub>6.84</sub>Nb<sub>29.63</sub>Fe<sub>5.822</sub>C<sub>3</sub> is 2.13 wt % at 3 MPa hydrogen pressure at 100 °C. This paper provides a design idea for doping C element in high entropy hydrogen storage alloys.</div></div>","PeriodicalId":18265,"journal":{"name":"Materials Research Bulletin","volume":"189 ","pages":"Article 113456"},"PeriodicalIF":5.3000,"publicationDate":"2025-03-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The phase ratio and thermal conductivity of TiVZrNbFe high entropy alloy were optimized by C doping to improve its hydrogen storage performance\",\"authors\":\"Sibo Wang , Hongkui Zhang , Zhen Wen , Yue Li , Tong Zhang , Yingdong Qu , Guanglong Li\",\"doi\":\"10.1016/j.materresbull.2025.113456\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>High entropy alloys (HEAs) have become a new type of hydrogen storage materials due to their extensive composition adjustability and unique high entropy effect, and have important application potential. Based on <strong>TiVZrNbFe</strong> high entropy alloys doped C element, the alloy integral replacement, finally was prepared (Ti<sub>30.55</sub>V<sub>25.85</sub>Zr<sub>7.05</sub>Nb<sub>30.55</sub>Fe<sub>6.00</sub>) <sub>1-x</sub>C<sub>x</sub> (<em>x</em> = 0.01,0.03,0.05,0.07,0.09) high entropy alloys. <strong>The results show that C element promotes the formation of C14 Laves phase, and the ratio of BCC phase to C14 Laves phase increases with the increase of carbon content.</strong> In addition, the C element in Ti<sub>29.63</sub>V<sub>25.08</sub>Zr<sub>6.84</sub>Nb<sub>29.63</sub>Fe<sub>5.822</sub>C<sub>3</sub> increased the thermal conductivity and decreased the apparent activation energy of hydrogen absorption. The hydrogen absorption capacity of Ti<sub>29.63</sub>V<sub>25.08</sub>Zr<sub>6.84</sub>Nb<sub>29.63</sub>Fe<sub>5.822</sub>C<sub>3</sub> is 2.13 wt % at 3 MPa hydrogen pressure at 100 °C. This paper provides a design idea for doping C element in high entropy hydrogen storage alloys.</div></div>\",\"PeriodicalId\":18265,\"journal\":{\"name\":\"Materials Research Bulletin\",\"volume\":\"189 \",\"pages\":\"Article 113456\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-03-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Materials Research Bulletin\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0025540825001643\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Research Bulletin","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0025540825001643","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
The phase ratio and thermal conductivity of TiVZrNbFe high entropy alloy were optimized by C doping to improve its hydrogen storage performance
High entropy alloys (HEAs) have become a new type of hydrogen storage materials due to their extensive composition adjustability and unique high entropy effect, and have important application potential. Based on TiVZrNbFe high entropy alloys doped C element, the alloy integral replacement, finally was prepared (Ti30.55V25.85Zr7.05Nb30.55Fe6.00) 1-xCx (x = 0.01,0.03,0.05,0.07,0.09) high entropy alloys. The results show that C element promotes the formation of C14 Laves phase, and the ratio of BCC phase to C14 Laves phase increases with the increase of carbon content. In addition, the C element in Ti29.63V25.08Zr6.84Nb29.63Fe5.822C3 increased the thermal conductivity and decreased the apparent activation energy of hydrogen absorption. The hydrogen absorption capacity of Ti29.63V25.08Zr6.84Nb29.63Fe5.822C3 is 2.13 wt % at 3 MPa hydrogen pressure at 100 °C. This paper provides a design idea for doping C element in high entropy hydrogen storage alloys.
期刊介绍:
Materials Research Bulletin is an international journal reporting high-impact research on processing-structure-property relationships in functional materials and nanomaterials with interesting electronic, magnetic, optical, thermal, mechanical or catalytic properties. Papers purely on thermodynamics or theoretical calculations (e.g., density functional theory) do not fall within the scope of the journal unless they also demonstrate a clear link to physical properties. Topics covered include functional materials (e.g., dielectrics, pyroelectrics, piezoelectrics, ferroelectrics, relaxors, thermoelectrics, etc.); electrochemistry and solid-state ionics (e.g., photovoltaics, batteries, sensors, and fuel cells); nanomaterials, graphene, and nanocomposites; luminescence and photocatalysis; crystal-structure and defect-structure analysis; novel electronics; non-crystalline solids; flexible electronics; protein-material interactions; and polymeric ion-exchange membranes.