{"title":"弥散强化Ni-Co合金的蠕变","authors":"J. Hancock, I. Dillamore, R. Smallman","doi":"10.1179/030634572790445867","DOIUrl":null,"url":null,"abstract":"AbstractThe creep behaviour of three Ni–Co–2.5% A12O3 alloys containing 0, 30) and 67% Co has been studied at temperatures in the region of 770 and 1000 K. It is shown that in both ranges the steady-state creep rate depends upon stress to the power four. At the lower temperature the activation energy is composition-dependent, values of 85, 184, and 121 kJ/mol being recorded for the 0, 30, and 67% Co alloys, respectively. At the higher temperature the activation energy corresponds with that for self-diffusion and, like the pre-exponential term, is essentially independent of composition except through small variations in diffusivity. The low-temperature creep is explained in terms of a thermally activated cross-slip and pipe-diffusion mechanism that enables dislocations to by-pass particles. At the higher temperature it is suggested that bulk diffusion is the rate-controlling process and that the absence of any marked composition-dependence is due to the jog distribution being determined mainly by dislocati...","PeriodicalId":103313,"journal":{"name":"Metal Science Journal","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":"{\"title\":\"The Creep of Dispersion-Strengthened Ni–Co Alloys\",\"authors\":\"J. Hancock, I. Dillamore, R. Smallman\",\"doi\":\"10.1179/030634572790445867\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"AbstractThe creep behaviour of three Ni–Co–2.5% A12O3 alloys containing 0, 30) and 67% Co has been studied at temperatures in the region of 770 and 1000 K. It is shown that in both ranges the steady-state creep rate depends upon stress to the power four. At the lower temperature the activation energy is composition-dependent, values of 85, 184, and 121 kJ/mol being recorded for the 0, 30, and 67% Co alloys, respectively. At the higher temperature the activation energy corresponds with that for self-diffusion and, like the pre-exponential term, is essentially independent of composition except through small variations in diffusivity. The low-temperature creep is explained in terms of a thermally activated cross-slip and pipe-diffusion mechanism that enables dislocations to by-pass particles. At the higher temperature it is suggested that bulk diffusion is the rate-controlling process and that the absence of any marked composition-dependence is due to the jog distribution being determined mainly by dislocati...\",\"PeriodicalId\":103313,\"journal\":{\"name\":\"Metal Science Journal\",\"volume\":\"10 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Metal Science Journal\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1179/030634572790445867\",\"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/10.1179/030634572790445867","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
AbstractThe creep behaviour of three Ni–Co–2.5% A12O3 alloys containing 0, 30) and 67% Co has been studied at temperatures in the region of 770 and 1000 K. It is shown that in both ranges the steady-state creep rate depends upon stress to the power four. At the lower temperature the activation energy is composition-dependent, values of 85, 184, and 121 kJ/mol being recorded for the 0, 30, and 67% Co alloys, respectively. At the higher temperature the activation energy corresponds with that for self-diffusion and, like the pre-exponential term, is essentially independent of composition except through small variations in diffusivity. The low-temperature creep is explained in terms of a thermally activated cross-slip and pipe-diffusion mechanism that enables dislocations to by-pass particles. At the higher temperature it is suggested that bulk diffusion is the rate-controlling process and that the absence of any marked composition-dependence is due to the jog distribution being determined mainly by dislocati...