{"title":"锌双晶的“纯”晶界滑动","authors":"C. Horton, N. Thompson, C. Beevers","doi":"10.1179/030634568790443486","DOIUrl":null,"url":null,"abstract":"AbstractBicrystals of zinc containing basal tilt boundaries of controlled orientation have been tested in simple shear over the range 320–390° C. Rapid grain-boundary sliding was observed in the absence of macroscopic trans crystalline slip. This “pure” grain-boundary sliding was accompanied by the emission of dislocations from the sliding boundaries and the creation of substructure in the crystalline regions adjacent to the boundaries. Grain-boundary slide-hardening was often noted in the absence of observable grain-boundary cusps or irregularities. By assuming a sliding-rate law of the form έ = Aσnt(m−1) exp( − Qs/KT) and by using differential test methods, values were obtained for the apparent activation energy (Qs ) and the stress parameter (n) for the “pure” grain-boundary sliding. The values Qs = 31 ± 5 (kcal/mole) and n = 4.5 ± 1.8 give strong support to the general conclusion that “pure” grain-boundary sliding is controlled by the case with which dislocations can be emitted by a sliding boundary a...","PeriodicalId":103313,"journal":{"name":"Metal Science Journal","volume":"48 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"13","resultStr":"{\"title\":\"“Pure” Grain-Boundary Sliding in Zinc Bicrystals\",\"authors\":\"C. Horton, N. Thompson, C. Beevers\",\"doi\":\"10.1179/030634568790443486\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"AbstractBicrystals of zinc containing basal tilt boundaries of controlled orientation have been tested in simple shear over the range 320–390° C. Rapid grain-boundary sliding was observed in the absence of macroscopic trans crystalline slip. This “pure” grain-boundary sliding was accompanied by the emission of dislocations from the sliding boundaries and the creation of substructure in the crystalline regions adjacent to the boundaries. Grain-boundary slide-hardening was often noted in the absence of observable grain-boundary cusps or irregularities. By assuming a sliding-rate law of the form έ = Aσnt(m−1) exp( − Qs/KT) and by using differential test methods, values were obtained for the apparent activation energy (Qs ) and the stress parameter (n) for the “pure” grain-boundary sliding. The values Qs = 31 ± 5 (kcal/mole) and n = 4.5 ± 1.8 give strong support to the general conclusion that “pure” grain-boundary sliding is controlled by the case with which dislocations can be emitted by a sliding boundary a...\",\"PeriodicalId\":103313,\"journal\":{\"name\":\"Metal Science Journal\",\"volume\":\"48 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"13\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Metal Science Journal\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1179/030634568790443486\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Metal Science Journal","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1179/030634568790443486","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
AbstractBicrystals of zinc containing basal tilt boundaries of controlled orientation have been tested in simple shear over the range 320–390° C. Rapid grain-boundary sliding was observed in the absence of macroscopic trans crystalline slip. This “pure” grain-boundary sliding was accompanied by the emission of dislocations from the sliding boundaries and the creation of substructure in the crystalline regions adjacent to the boundaries. Grain-boundary slide-hardening was often noted in the absence of observable grain-boundary cusps or irregularities. By assuming a sliding-rate law of the form έ = Aσnt(m−1) exp( − Qs/KT) and by using differential test methods, values were obtained for the apparent activation energy (Qs ) and the stress parameter (n) for the “pure” grain-boundary sliding. The values Qs = 31 ± 5 (kcal/mole) and n = 4.5 ± 1.8 give strong support to the general conclusion that “pure” grain-boundary sliding is controlled by the case with which dislocations can be emitted by a sliding boundary a...