Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C
High-pressure sliding (HPS) and rotary swaging (RS) at room temperature were used to form severely deformed microstructures in martensitic creep-resistant P92 steel. The deformed microstructures contained markedly different ratios of low- and high-angle grain boundaries (LAGBs/HAGBs). The applicatio...
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2021-12-01
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author | Petr Kral Jiri Dvorak Vaclav Sklenicka Zenji Horita Yoichi Takizawa Yongpeng Tang Lenka Kunčická Marie Kvapilova Marie Ohankova |
author_facet | Petr Kral Jiri Dvorak Vaclav Sklenicka Zenji Horita Yoichi Takizawa Yongpeng Tang Lenka Kunčická Marie Kvapilova Marie Ohankova |
author_sort | Petr Kral |
collection | DOAJ |
description | High-pressure sliding (HPS) and rotary swaging (RS) at room temperature were used to form severely deformed microstructures in martensitic creep-resistant P92 steel. The deformed microstructures contained markedly different ratios of low- and high-angle grain boundaries (LAGBs/HAGBs). The application of the RS method, with an imposed equivalent strain of 1.4, led to the formation of a heterogeneous microstructure with a high number of LAGBs, while the HPS method, with an imposed equivalent strain of 7.8, led to the formation of a relatively homogeneous ultrafine-grained microstructure with a significant predominance of HAGBs. Microstructure analyses after creep testing showed that the microstructure of RS- and HPS-processed P92 steel is quite stable, but a slight coarsening of subgrains and grains during creep testing can be observed. Constant load tensile creep tests at 500 °C and initial stresses ranging from 300 to 900 MPa revealed that the specimens processed by HPS exhibited higher creep strength (slower minimum creep rate) and ductility compared to the coarse-grained and RS-processed P92 steel. However, the HPS-processed P92 steel also exhibited lower values of stress exponent n than the other investigated states of P92 steel. For this reason, the differences in minimum creep rates determined for different states decrease with decreasing values of applied stress, and at applied stresses lower than 500 MPa, the creep resistance of the RS-processed state is higher than the creep resistance of the HPS-processed state. |
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spelling | doaj.art-feac514b7b114896aed889aa9b2926422023-11-23T09:34:42ZengMDPI AGMetals2075-47012021-12-011112204410.3390/met11122044Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °CPetr Kral0Jiri Dvorak1Vaclav Sklenicka2Zenji Horita3Yoichi Takizawa4Yongpeng Tang5Lenka Kunčická6Marie Kvapilova7Marie Ohankova8Czech Academy of Sciences, Institute of Physics of Materials, 616 00 Brno, Czech RepublicCzech Academy of Sciences, Institute of Physics of Materials, 616 00 Brno, Czech RepublicCzech Academy of Sciences, Institute of Physics of Materials, 616 00 Brno, Czech RepublicDepartment of Engineering, Kyushu Institute of Technology, Kitakyushu 804-8550, JapanTechnology Department, Nagano Forging Co., Ltd., Nagano 381-0003, JapanDepartment of Engineering, Kyushu Institute of Technology, Kitakyushu 804-8550, JapanCzech Academy of Sciences, Institute of Physics of Materials, 616 00 Brno, Czech RepublicCzech Academy of Sciences, Institute of Physics of Materials, 616 00 Brno, Czech RepublicUJP PRAHA a.s., Zbraslav, 156 10 Praha, Czech RepublicHigh-pressure sliding (HPS) and rotary swaging (RS) at room temperature were used to form severely deformed microstructures in martensitic creep-resistant P92 steel. The deformed microstructures contained markedly different ratios of low- and high-angle grain boundaries (LAGBs/HAGBs). The application of the RS method, with an imposed equivalent strain of 1.4, led to the formation of a heterogeneous microstructure with a high number of LAGBs, while the HPS method, with an imposed equivalent strain of 7.8, led to the formation of a relatively homogeneous ultrafine-grained microstructure with a significant predominance of HAGBs. Microstructure analyses after creep testing showed that the microstructure of RS- and HPS-processed P92 steel is quite stable, but a slight coarsening of subgrains and grains during creep testing can be observed. Constant load tensile creep tests at 500 °C and initial stresses ranging from 300 to 900 MPa revealed that the specimens processed by HPS exhibited higher creep strength (slower minimum creep rate) and ductility compared to the coarse-grained and RS-processed P92 steel. However, the HPS-processed P92 steel also exhibited lower values of stress exponent n than the other investigated states of P92 steel. For this reason, the differences in minimum creep rates determined for different states decrease with decreasing values of applied stress, and at applied stresses lower than 500 MPa, the creep resistance of the RS-processed state is higher than the creep resistance of the HPS-processed state.https://www.mdpi.com/2075-4701/11/12/2044creep-resistant steelssevere plastic deformationcreep behavior |
spellingShingle | Petr Kral Jiri Dvorak Vaclav Sklenicka Zenji Horita Yoichi Takizawa Yongpeng Tang Lenka Kunčická Marie Kvapilova Marie Ohankova Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C Metals creep-resistant steels severe plastic deformation creep behavior |
title | Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C |
title_full | Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C |
title_fullStr | Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C |
title_full_unstemmed | Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C |
title_short | Influence of High Pressure Sliding and Rotary Swaging on Creep Behavior of P92 Steel at 500 °C |
title_sort | influence of high pressure sliding and rotary swaging on creep behavior of p92 steel at 500 °c |
topic | creep-resistant steels severe plastic deformation creep behavior |
url | https://www.mdpi.com/2075-4701/11/12/2044 |
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