scholarly journals Effect of tempering temperature on the microstructure and creep resistance of a 10%Cr martensitic steel

2021 ◽  
Vol 1014 (1) ◽  
pp. 012027
Author(s):  
R V Mishnev ◽  
N R Dudova ◽  
R O Kaibyshev
2015 ◽  
Vol 645-646 ◽  
pp. 427-434
Author(s):  
Jian Min Wang ◽  
Wen Tao Hou ◽  
Lin Lu

A new technology of preparing submicron medium-carbon steel quickly using martensitic steel by equal-channel angular pressing is developed. The technology combines martensite phase transformation with severe plastic deformation. In this research, martensitic steel is heated to 923K quickly and held for appropriate time, then equal-channel angular pressing is implemented. Supersaturated ferrites of average grain size within 0.5μm are obtained by the interaction of dislocation intersection, dynamic recrystallization and strain-induced phase transformation. At the same time, strain-induced phase transformation leads to dispersive precipitation of supersaturated carbon particles in the form of carbide inside grains or in grain boundaries. The optimal size of ferrite grains and the optimal distribution of carbides are acquired by controlling tempering temperature and time. The results show that ultra-fine grained materials prepared by this technology possess superior thermal stability.


2016 ◽  
Vol 678 ◽  
pp. 178-189 ◽  
Author(s):  
R. Mishnev ◽  
N. Dudova ◽  
A. Fedoseeva ◽  
R. Kaibyshev

2019 ◽  
Vol 8 (5) ◽  
pp. 4588-4597 ◽  
Author(s):  
Yingxue Chen ◽  
Zhiyuan Hong ◽  
Xiaoxin Zhang ◽  
Min Xia ◽  
Qingzhi Yan ◽  
...  

2014 ◽  
Vol 455 (1-3) ◽  
pp. 496-499 ◽  
Author(s):  
N.A. Polekhina ◽  
I.Yu. Litovchenko ◽  
A.N. Tyumentsev ◽  
Е.G. Astafurova ◽  
V.M. Chernov ◽  
...  

Materials ◽  
2017 ◽  
Vol 10 (4) ◽  
pp. 388 ◽  
Author(s):  
Josip Brnic ◽  
Sanjin Krscanski ◽  
Domagoj Lanc ◽  
Marino Brcic ◽  
Goran Turkalj ◽  
...  

2010 ◽  
Vol 400 (1) ◽  
pp. 94-102 ◽  
Author(s):  
Yin Zhong Shen ◽  
Sung Ho Kim ◽  
Hai Dong Cho ◽  
Chang Hee Han ◽  
Woo Seog Ryu

2016 ◽  
Vol 22 (4) ◽  
pp. 266 ◽  
Author(s):  
Andrea Di Schino

<p>The microstructural evolution of a quenched and tempered medium-C micro-alloyed steel during tempering is analyzed The steel was heat treated in order to develop fully martensitic microstructures after quenching with different prior austenite grain sizes (AGS).</p><p>Main results can be summarized as below:</p><ul><li>A very poor effect of AGS on packet size is found.</li><li>High-angle boundary grains do not significantly grow after tempering; on the contrary, low-angle grain boundaries (cells) move, fully justifying the hardness evolution with tempering temperature. </li></ul>


Magnetoacoustic emission (MAE) and Barkhausen emission (BE) have been measured as a function of applied magnetic field and tensile stress from mild-steel samples in a wide range of heat treatments, to develop a technique to measure stress without prior knowledge of the microstructure. The results are supplemented by measurements of magnetic coercivity and mechanical hardness. MAE is found to decrease with increasing applied stress, whereas the variation of BE is more complicated. The amplitudes of both MAE and BE, as well as the coercivity and hardness are also found to depend on the microstructure to varying degrees. Thus in ferritic-pearlitic and ferritic-pearlitic-martensitic steel MAE is much more sensitive to stress than to changes in microstructure, whereas the sensitivity of BE to stress and microstructure is similar. Above 50 MPa MAE is also more sensitive to stress in ferrite containing cementite, whereas BE both lacks a monotonic dependence upon stress and is sensitive to microstructure. In martensite, however, there is no MAE, the BE increasing monotonically with stress. Tempered martensitic structures give a weak MAE signal that is more sensitive to tempering temperature than applied stress, whereas the BE increases with stress for tempers below 500°C and decreases above. The dependence of MAE and BE on magnetic field are discussed in terms of domain-wall nucleation and irreversible motion in ferrite at higher fields, and irreversible wall motion through martensite or pearlite at lower fields. The results imply that MAE can be used alone to measure stress provided the general form of the microstructure is known; otherwise BE can be used as an additional technique to resolve any ambiguity.


2011 ◽  
Vol 417 (1-3) ◽  
pp. 29-32 ◽  
Author(s):  
Manabu Tamura ◽  
Takuya Kumagai ◽  
Kazuhisa Sakai ◽  
Kei Shinozuka ◽  
Hisao Esaka

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