Hot Deformation Behavior of V-Microalloyed Steel
Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel,the continuous cooling transformation curve was obtained.The influence on steel microstructure and hardness at different cooling rates was stu...
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| Published in | Journal of iron and steel research, international Vol. 17; no. 8; pp. 55 - 60 |
|---|---|
| Main Authors | , , , , , |
| Format | Journal Article |
| Language | English |
| Published |
Singapore
Elsevier Ltd
01.08.2010
Springer Singapore |
| Subjects | |
| Online Access | Get full text |
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| Abstract | Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel,the continuous cooling transformation curve was obtained.The influence on steel microstructure and hardness at different cooling rates was studied.The softening behavior of isothermal deforming in austenite area of 850-1000 ℃ in the interval of passes was also studied by double-pass compression test.The results show that the product of austenite transformation is pearlite when the cooling rate is lower than 10 ℃.When the cooling rate was in the range of 10-50 ℃·s-1,only martensite was received.The hardness of the test steel increases with increasing the cooling rate.Under the condition of deformation of 30% and deformation rate of 3 s-1,the relaxation time for complete recrystallization was shorter than 100 s when deformation temperature was higher than 1000 ℃.When deformation temperature was lower than 880 ℃,complete recrystallization of steel was difficult to achieve even if the relaxation time is extended. |
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| AbstractList | Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel, the continuous cooling transformation curve was obtained. The influence on steel microstructure and hardness at different cooling rates was studied. The softening behavior of isothermal deforming in austenite area of 850—1000 °C in the interval of passes was also studied by double-pass compression test. The results show that the product of austenite transformation is pearlite when the cooling rate is lower than 10 °C. When the cooling rate was in the range of 10 — 50 °C • s
−1
, only martensite was received. The hardness of the test steel increases with increasing the cooling rate. Under the condition of deformation of 30% and deformation rate of 3 s
−1
, the relaxation time for complete recrystallization was shorter than 100 s when deformation temperature was higher than 1000 °C. When deformation temperature was lower than 880 °C, complete recrystallization of steel was difficult to achieve even if the relaxation time is extended. Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel, the continuous cooling transformation curve was obtained. The influence on steel microstructure and hardness at different cooling rates was studied. The softening behavior of isothermal deforming in austenite area of 850-1000 degree C in the interval of passes was also studied by double-pass compression test. The results show that the product of austenite transformation is pearlite when the cooling rate is lower than 10 degree C. When the cooling rate was in the range of 10-50 degree C super(. s) super(-)1 only martensite was received. The hardness of the test steel increases with increasing the cooling rate. Under the condition of deformation of 30% and deformation rate of 3 s super(-1), the relaxation time for complete recrystallization was shorter than 100 s when deformation temperature was higher than 1000 C. When deformation temperature was lower than 880 degree C, complete recrystallization of steel was difficult to achieve even if the relaxation time is extended. Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel,the continuous cooling transformation curve was obtained.The influence on steel microstructure and hardness at different cooling rates was studied.The softening behavior of isothermal deforming in austenite area of 850-1000 ℃ in the interval of passes was also studied by double-pass compression test.The results show that the product of austenite transformation is pearlite when the cooling rate is lower than 10 ℃.When the cooling rate was in the range of 10-50 ℃·s-1,only martensite was received.The hardness of the test steel increases with increasing the cooling rate.Under the condition of deformation of 30% and deformation rate of 3 s-1,the relaxation time for complete recrystallization was shorter than 100 s when deformation temperature was higher than 1000 ℃.When deformation temperature was lower than 880 ℃,complete recrystallization of steel was difficult to achieve even if the relaxation time is extended. Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel, the continuous cooling transformation curve was obtained. The influence on steel microstructure and hardness at different cooling rates was studied. The softening behavior of isothermal deforming in austenite area of 850–1000 °C in the interval of passes was also studied by double-pass compression test. The results show that the product of austenite transformation is pearlite when the cooling rate is lower than 10 °C. When the cooling rate was in the range of 10–50 °C · s −1, only martensite was received. The hardness of the test steel increases with increasing the cooling rate. Under the condition of deformation of 30% and deformation rate of 3 s −1, the relaxation time for complete recrystallization was shorter than 100 s when deformation temperature was higher than 1000 C. When deformation temperature was lower than 880 °C, complete recrystallization of steel was difficult to achieve even if the relaxation time is extended. |
| Author | REN An-chao JI Yu ZHOU Gui-feng YUAN Ze-xi HAN Bin LI Yi |
| AuthorAffiliation | Institute of Material Science and Metallurgy, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China Research and Development Center, Wuhan Iron and Steel （Group） Co, Wuhan 430080, Hubei, China International Trade Company, Wuhan Iron and Steel （Group） Co, Wuhan 430080, Hubei, China |
| Author_xml | – sequence: 1 givenname: An-chao surname: REN fullname: REN, An-chao email: anchaoren@163.com organization: Institute of Material Science and Metallurgy, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China – sequence: 2 givenname: Yu surname: JI fullname: JI, Yu organization: Research and Development Center, Wuhan Iron and Steel (Group) Co, Wuhan 430080, Hubei, China – sequence: 3 givenname: Gui-feng surname: ZHOU fullname: ZHOU, Gui-feng organization: Institute of Material Science and Metallurgy, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China – sequence: 4 givenname: Ze-xi surname: YUAN fullname: YUAN, Ze-xi organization: Institute of Material Science and Metallurgy, Wuhan University of Science and Technology, Wuhan 430081, Hubei, China – sequence: 5 givenname: Bin surname: HAN fullname: HAN, Bin organization: Research and Development Center, Wuhan Iron and Steel (Group) Co, Wuhan 430080, Hubei, China – sequence: 6 givenname: Yi surname: LI fullname: LI, Yi organization: International Trade Company, Wuhan Iron and Steel (Group) Co, Wuhan 430080, Hubei, China |
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| Cites_doi | 10.2355/isijinternational.41.542 10.1007/BF02647973 10.1016/S0956-716X(99)80009-0 10.2355/isijinternational.42.423 10.1016/j.scriptamat.2005.03.014 10.1016/0924-0136(96)02392-8 10.1007/BF02649763 10.2355/isijinternational.41.63 10.1016/S0167-577X(02)00440-8 10.1007/BF02648589 10.1016/0956-7151(92)90006-Z 10.1016/S1359-6462(98)00452-7 10.2355/isijinternational.33.1257 10.1016/S1359-6454(00)00389-X 10.2355/isijinternational.35.1523 |
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| Copyright | 2010 Central Iron and Steel Research Institute China Iron and Steel Research Institute Group 2010 |
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| Keywords | static recrystallization U75V rail steel thermal simulation deformation temperature continuous cooling transformation curve |
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| Notes | 11-3678/TF U75V rail steel continuous cooling transformation curve TQ323.4 static recrystallization thermal simulation TG142.33 deformation temperature U75V rail steel; thermal simulation; continuous cooling transformation curve; deformation temperature; static recrystallization ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
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| PublicationTitle | Journal of iron and steel research, international |
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| Snippet | Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail... Through the expansion curve of continuous cooling transformation at different cooling rates measured by THERMECMASTOR-Z thermal simulator for U75V rail steel,... |
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| SubjectTerms | Applied and Technical Physics continuous cooling transformation curve Cooling rate Deformation deformation temperature Engineering Iron and steel industry Machines Manufacturing Materials Engineering Materials Science Metallic Materials Physical Chemistry Processes Recrystallization Relaxation time static recrystallization Steel making Structural steels thermal simulation Transformations U75V rail steel 冷却速度 压缩试验 变形温度 奥氏体转变 弛豫时间 微合金化钢 热变形行为 连续冷却转变曲线 |
| Title | Hot Deformation Behavior of V-Microalloyed Steel |
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