Continuous Cooling Transformation of Overcooling Austenite and Structure Fining of 0.33C-1.0Mn-0.8Si Steel
|更新时间:2026-01-21
|
Continuous Cooling Transformation of Overcooling Austenite and Structure Fining of 0.33C-1.0Mn-0.8Si Steel
Special SteelVol. 30, Issue 2, Pages: 55-57(2009)
作者机构:
河北理工大学金属材料工程系,唐山,063009
作者简介:
基金信息:
DOI:
CLC:
Received:08 September 2008,
Online First:05 December 2022,
Published:05 December 2009
稿件说明:
移动端阅览
冯运莉, 杨晓彩, 张宁宁. Continuous Cooling Transformation of Overcooling Austenite and Structure Fining of 0.33C-1.0Mn-0.8Si Steel[J]. Special Steel, 2009, 30(2): 55-57.
DOI:
冯运莉, 杨晓彩, 张宁宁. Continuous Cooling Transformation of Overcooling Austenite and Structure Fining of 0.33C-1.0Mn-0.8Si Steel[J]. Special Steel, 2009, 30(2): 55-57.DOI:
Continuous Cooling Transformation of Overcooling Austenite and Structure Fining of 0.33C-1.0Mn-0.8Si Steel
Static (non-deformation) and dynamic (deformation) continuous cooling transformation (CCT) curves of steel0.33C-1.0Mn-0.8Si was measured by Gleeble-3500 thermo-mechanical simulator
and structure of steel was observed. Results showed that the deformation of overcooling austenite could increase initial transformation temperature of ferrite
but had no obvious influence on temperature of completion of transformation
the zone of ferrite transformation of deformed overcooling austenite enlarged
and Ar
3
value for deformed austenite was higher by 100 ℃ than that for non-deformed austenite while effect of deformation on Ar
1
was no-obvious; and with increasing cooling rate
the morphology of fer- rite grain changed from polygonal to lath and long leaf structure and the pearlite colonies became more fine and dispersed
and the continuous cooling structure fo
r deformed austenite was finer than that for non-deformed austenite.