{"title":"压缩铜的织构和显微组织","authors":"C. Lee, C. Lee, R. Smallman","doi":"10.1155/TSM.26-27.137","DOIUrl":null,"url":null,"abstract":"It is shown that the deformation banding tendency in copper increases as deformation temperature \nincreases. After 70% compression, the average number of deformation bands per grain increases from \n16 to 36 as the deformation temperature increases from 25 to 300℃. An orientation dependence of \nbanding tendency is also observed. Grains with near {110} orientation are found to have the lowest \nbanding tendency. The textures of samples compressed below 300℃ are similar and consist mainly \nof a {110} fibre and a weak {100} fibre. While the {110} component remains when deformation \ntemperature is increased to 300℃; the {100} component becomes weaker. 300℃ is in fact the temperature at which large scale dynamic recrystallisation occurs. It is suspected that the decay of the \n{100} component is due to dynamic recrystallisation which takes place preferentially at thin deformation \nbands where most of the {100} oriented material is found.","PeriodicalId":413822,"journal":{"name":"Texture, Stress, and Microstructure","volume":"31 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Texture and Microstructure of Compressed Copper\",\"authors\":\"C. Lee, C. Lee, R. Smallman\",\"doi\":\"10.1155/TSM.26-27.137\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It is shown that the deformation banding tendency in copper increases as deformation temperature \\nincreases. After 70% compression, the average number of deformation bands per grain increases from \\n16 to 36 as the deformation temperature increases from 25 to 300℃. An orientation dependence of \\nbanding tendency is also observed. Grains with near {110} orientation are found to have the lowest \\nbanding tendency. The textures of samples compressed below 300℃ are similar and consist mainly \\nof a {110} fibre and a weak {100} fibre. While the {110} component remains when deformation \\ntemperature is increased to 300℃; the {100} component becomes weaker. 300℃ is in fact the temperature at which large scale dynamic recrystallisation occurs. It is suspected that the decay of the \\n{100} component is due to dynamic recrystallisation which takes place preferentially at thin deformation \\nbands where most of the {100} oriented material is found.\",\"PeriodicalId\":413822,\"journal\":{\"name\":\"Texture, Stress, and Microstructure\",\"volume\":\"31 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Texture, Stress, and Microstructure\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1155/TSM.26-27.137\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Texture, Stress, and Microstructure","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1155/TSM.26-27.137","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
It is shown that the deformation banding tendency in copper increases as deformation temperature
increases. After 70% compression, the average number of deformation bands per grain increases from
16 to 36 as the deformation temperature increases from 25 to 300℃. An orientation dependence of
banding tendency is also observed. Grains with near {110} orientation are found to have the lowest
banding tendency. The textures of samples compressed below 300℃ are similar and consist mainly
of a {110} fibre and a weak {100} fibre. While the {110} component remains when deformation
temperature is increased to 300℃; the {100} component becomes weaker. 300℃ is in fact the temperature at which large scale dynamic recrystallisation occurs. It is suspected that the decay of the
{100} component is due to dynamic recrystallisation which takes place preferentially at thin deformation
bands where most of the {100} oriented material is found.