Abstract
High nitrogen stainless steel has excellent mechanical and chemical properties. Cr-Mn-Mo high nitrogen stainless steel with a nitrogen content of 0.54wt% was smelted by increasing the content of Cr and Mn at the nitrogen partial pressure of 80 000 Pa. The sample steels after hot rolling were held at 800, 900, 1000, 1100 and 1200 °C for 1, 2, 3, 4, and 5 h. Orthogonal analysis was carried out to study the microstructure, yield strength, tensile strength, elongation to fracture, reduction of area, and product of strength and plasticity under different temperatures and holding time, in order to find the best heat treatment temperature and time for the test steel. The results show that Cr2N precipitates in the samples without solution treatment and after solution treatment at 800 and 900 °C, and ferrite precipitates in the samples after solution treatment at 1200 °C. The materials treated at 1000 and 1100 °C are pure austenite. The specimen held at 1000 °C for 4 h has the best plasticity and high strength, and its section shrinkage and post-fracture elongation can reach 67.5% and 69.5%, respectively. The strength of the samples without heat treatment is the highest, and the reduction of section and elongation after fracture remains at 42% and 49.9%. The comprehensive mechanical properties of the samples held at 1000 °C for 1 h are the best, and the product of strength and plasticity can reach 58.59 GPa%.
Science Press
With the development of science and technology, stainless steel is required to have the characteristics of high-cost performance, green and environmental safety, and the development of low-cost stainless steel with good comprehensive performance is of great significance to the development of the steel industry. Because Ni is scarce and expensive and is harmful to the human body, researchers have replaced the rare and expensive Ni elements with inexpensive N and Mn elements, and Cr-Mn series high-nitrogen stainless steels have been successively develope
The tested steel was smelted with industrial pure iron, electrolytic manganese, pure chromium, ferromolybdenum, nitrogen-manganese alloy, and nitrogen-chromium alloy in a 50 kg vacuum induction furnace at a nitrogen partial pressure of 80 000 Pa and a temperature of 1550 °C, and a small amount of aluminum was added for de-oxidation. After tapping, it is cooled to room temperature with the furnace to form a 150 mm×150 mm square billet. After electroslag remelting, the chemical composition of the material is shown in
The 10 mm×10 mm metallographic specimens and standard tensile specimens of the hot-rolled sheet are shown in

Fig.1 Tensile spcimen structure drawing

FactSage software was used to calculate the phase diagram of the alloy, as shown in Fig.2. Fig.2 shows that the alloy is a single austenite phase at 920~1124 °C; when the temperature is higher than 1124 °C, the ferrite phase is gradually precipitated from the austenite; when the temperature is lower than 920 °C, the close-packed hexagonal crystals phase is gradually precipitated from the austenite. After XRD analysis, it can be determined that the precipitated close-packed hexagonal crystals phase is Cr2N.

Fig.3 XRD patterns of test steels held at room temperature (a) and 800, 900, 1000, 1100 and 1200 °C for 1 (b), 3 (c), and 5 h (d)

Fig.4 Microscopic structures of test steel solution treated under different conditions: (a) untreated; (b, c, d) 800 ℃; (e, f, g) 900 ℃; (h, i, j) 1000 ℃; (k, l, m) 1100 ℃; (n, o, p) 1200 ℃; (b, e, h, k, n) 1 h; (c, f, i, l, o) 3 h; (d, g, j, m, p) 5 h

Fig.5 Grain size of test steels after holding at different temperatures for 1 h
In summary, with the increase of the holding temperature, the crystal grains gradually become larger, the grain boundary density and twin crystals gradually decrease. This is because high temperature promotes the growth and reorganization of the crystal grains. At room temperature, 800 and 900 °C, it is an austenite structure with a small amount of Cr2N precipitation. The precipitation of Cr2N inhibits the growth of grains to a certain extent, so the grains grow slowly below 900 °C; at 1000 and 1100 °C, Cr2N dissolves into the austenite, and the grains grow quickly which are fully austenitic structures. When the temperature reaches 1200 °C, ferrite will begin to precipitate from the austenite, which is basically consistent with the phase diagram in Fig.2.

Fig.6 Effect of holding time on average grain size of test steels
Tensile tests were carried out on test steels with different solution treatment temperatures at room temperature to reveal the influence of different solution treatment temperatures on the mechanical properties of the test steels. To show the effect of heat treatment temperature on the strength and plasticity of the material more intuitively, the composite alloy was heated to 800, 900, 1000, and 1100, 1200 °C for 1, 2, 3, 4, and 5 h, and then water cooled to room temperature. After the stretching data, the Origin software was used to obtain to

Fig.7 Tensile strength (a) and yield strength (b) of test steels after solution treatment at different temperatures

Fig.8 Elongation (a) and reduction of area (b) of test steels after solution treatment at different temperatures
In the process of plastic deformation of steel materials, the main way is the slip of dislocations. The grain boundary has an obstructive effect on the slip of dislocations. The fine grains have a large number of dislocations, which hinder dislocation movement. It has a greater effect and can significantly increase the strength of steel; fine precipitates (ferrite, Cr2N) increase the distortion of the crystal lattice, have a pinning effect on the slip of dislocations, and can increase the strength of steel.
At room temperature, the crystal grains are extremely small, the grain boundary density is extremely high, and the strength is the highest; although a small amount of Cr2N precipitates at 800 °C which play a role of strengthening the second phase, the increase in grain size and the decrease in grain boundary density still dominate, making the strength slightly decrease; the strength decreases significantly at 800~1000 °C, which is due to the gradual dissolution of Cr2N as the holding temperature rises to the austenite phase region, so that the grain boundary density and the second phase precipitates are significantly reduced. At 1000~1100 °C, the growth of grains leads to a decrease in grain boundary density and reorganization of grains leads to a decrease in dislocations and twins, resulting in a slow decline in strength. At 1100~1200 °C, on the one hand, the grains grow, which reduces the strength, on the other hand, ferrite gradually precipitates from the austenite, and the second phase strengthening effect appears again, making the strength increase. The combined effect of two factors makes the intensity basically stable or even rise. When the holding time reaches more than 3 h, the austenite grains grow to the critical value and basically stop growing. At this time, the precipitation and growth of austenite ferrite play a pinning role to a certain extent, so the strength increases.

Fig.9 Tensile strength (a) and yield strength (b) of test steels after solution treatment at different temperatures for different time

Fig.10 Elongation (a) and reduction of area (b) of test steels after solution treatment at different temperatures for different time
The effect of solution time and temperature is displayed in

Fig.11 Combined effect of solution time and temperature on tensile strength (a), yield strength (b), elongation (c) and reduction of area (d)
1) With the increase of the solid solution temperature, the crystal grains gradually increase, and Cr2N precipitates at 800~900 °C, which is single austenite structure at 1000~1100 °C, and accompanied by ferrite at 1200 °C.
2) With the extension of the solution time, the crystal grains grow up and gradually stabilize, and the precipitates gradually increase and tend to balance.
3) As the solid solution temperature rises, the strength of the test steel gradually decreases, and the plasticity shows a trend of first rising and then falling, and the plasticity is the best at the austenite temperature.
4) With the extension of the solution time, the strength of the test steel shows a sharp decline first to a steady state. The plasticity at 800 and 900 °C declines first and then rises, and the extension of the holding time at 1000, 1100 and 1200 °C has an small effect on the plasticity.
5) The maximum yield strength and tensile strength of the test steel without solution treatment can reach 1157 and 884 MPa, respectively, and the plasticity of the sample after holding at 1000 °C for 4 h is the best, its elongation and reduction of the area can reach 67.5% and 69.5%, respectively. Sample treated at 1000 °C for 1 h has the optimal comprehensive mechanical properties. Its product of strength and plasticity can reach 58.59 GPa%.
References
Peter J Uggowitzer, Ruth Magdowski, Markus O Speidel. ISIJ International[J], 1996, 36(7): 901 [Baidu Scholar]
Speidel M O. Materialwissenschaft und Werkstofftechnik[J], 2006, 37(10): 875 [Baidu Scholar]
Vijayan Vijeesh, Ravichandran G, Rao Muralidhara et al. Journal of Failure Analysis and Prevention[J], 2021, 21: 976 [Baidu Scholar]
Yang D Q, Huang Y, Fan J K et al. Journal of Manufacturing Processes[J], 2021, 61: 261 [Baidu Scholar]
Ning X Z, Xing C J, Yong Q L et al. China Metallurgy[J], 2019, 29(5): 53 (in Chinese) [Baidu Scholar]
Grabke H J. ISIJ International[J], 1996, 36(7): 777 [Baidu Scholar]
Bannykh I O, Betsofen S Ya, Grushin I A et al. Russian Metallurgy (Metally)[J], 2020, 2020(10): 1122 [Baidu Scholar]
Yang Y, Tang W F. Key Engineering Materials[J], 2020, 6033: 89 [Baidu Scholar]
Zhou R, Northwood Derek O, Liu C. Journal of Materials Research and Technology[J], 2020, 9(2): 2331 [Baidu Scholar]
Ren Y B. Science of Advanced Materials[J], 2020, 12(1): 44 [Baidu Scholar]
Miao Cheng, Zhong Tao, Wu Hailing et al. Defence Technology[J], 2018, 14(5): 496 [Baidu Scholar]
Ren Shuai, Sun Zhiyan, Xu Zizhen et al. Journal of Materials Research[J], 2018, 33(12): 1764 [Baidu Scholar]
Shi F, Gao R H, Guan X J et al. Acta Metallurgica Sinica[J], 2020, 33(6): 789 [Baidu Scholar]
Zhang H, Xue P, Wang D et al. Journal of Materials Science & Technology[J], 2019, 35(7): 1278 [Baidu Scholar]
Jia Xiangdong, Zhao Yang, Xu Siqi. Rare Metal Materials and Engineering[J], 2021, 50(3): 963 (in Chinese) [Baidu Scholar]
Yang F B, Jing Y H, Li D et al. Rare Metals[J], 2018, 37(1): 35 [Baidu Scholar]
Yu Zhentao, Zhang Yafeng, Liu Hui et al. Rare Metal Materials and Engineering[J], 2010, 39(10): 1795 (in Chinese) [Baidu Scholar]
Zhao Y N, Jiang S Y, Zhang Y Q et al. Acta Metallurgica Sinica[J], 2017, 30(8): 762 [Baidu Scholar]
Gu Guiyue, Chen Feng, Zhang Qiang et al. Rare Metal Materials and Engineering[J], 2010, 39(4): 678 (in Chinese) [Baidu Scholar]
Lei R S, Wang M P. Acta Metallurgica Sinica[J], 2017, 30(12): 1155 [Baidu Scholar]
Zhang Jing, Yang Liang, Zuo Rulin. Rare Metal Materials and Engineering[J], 2015, 44(4): 956 (in Chinese) [Baidu Scholar]
Zhang X, Liu Q S. Acta Metallurgica Sinica[J], 2016, 29(9): 884 [Baidu Scholar]
Ma Xiong, Liang Xiaobo, Zhang Jianwei et al. Rare Metal Materials and Engineering[J], 2017, 46(S1): 109 (in Chinese) [Baidu Scholar]
Zhang W, Zhang X, Wang Q et al. Acta Metallurgica Sinica[J], 2018, 31(5): 471 [Baidu Scholar]