共查询到16条相似文献,搜索用时 78 毫秒
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通过对0.1mm厚的纯铁片在640~650℃气体渗氮的方法制备含氮量均匀的单一高氮奥氏体,其含氮量约为2.7wt.%。利用光学显微镜、X射线衍射和透射电子显微镜研究了高氮奥氏体中温转变后的显微组织,初步确定了高氮奥氏体中温转变产生高硬度的原因是由于晶内纳米级7'-Fe4N相的析出后,在晶内形成(α-Fe+γ/γ'-Fe4N)微纳级的晶粒,由这些微纳米颗粒引起的显微晶界强化是高氮奥氏体中温转变组织具超过常规时效强化的高硬度。 相似文献
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研究含氮量在(2.6—2.7)%wt范围的过饱和高氮奥氏体225℃中温转变过程中发现,Fe—N中温转变与Fe-C系中温贝氏体转变有明显不同。高氮奥氏体在225℃等温时首先析出γ‘‘-Fe4N,γ-Fe(N)与γ‘‘-Fe4N的亚稳定组织,等温1-2h后在含氮量降低的奥氏体中形成α-Fe,8-10h后分解成α-Fe,8-10h后分解成(α-Fe γ‘‘-Fe4N)的两相稳定组织,显微硬度最高可达l100HV0.025。分解后的两相组织品粒细小,使衍射蜂宽化,扫描电镜观察以及X-ray衍射分析表明:分解产物随等温时间延长粗化不明显。 相似文献
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采用OM,XRD,SEM和TEM研究了由纯铁穿透渗氮所得高氮奥氏体经225℃中温转变后的显微组织,确定了转变产物的种类和形态.等温转变属于γ→α-Fe γ'-Fe4N上贝氏体转变,转变产物由α-Fe板条和γ'-Fe4N板条交替排列而成的贝氏体板条团以及离散分布在贝氏体团块间的残余奥氏体(γr)小团块组成.该贝氏体相变在晶界和晶内位错线上优先形核、长大,具有扩散型相变的特征,其领先相是γ'-Fe4N.γ'-Fe4N与奥氏体晶体结构上的相似性及界面良好的共格性,保证了γ'-Fe4N从奥氏体的顺利析出. 相似文献
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对热轧态节镍型高氮奥氏体不锈钢进行固溶及时效处理,利用光学显微镜、电子背散射衍射,结合相图系统分析该材料固溶处理及时效后组织变化规律。结果表明,1050 ℃固溶处理后,试验钢基体为奥氏体,存在少量的铁素体,奥氏体晶粒形状偏等轴,晶粒内部存在大量孪晶。时效后,析出相主要为Cr2N、CrN、Cr23C6。在时效时间为5 h不变的条件下,温度由650 ℃升高至800 ℃,碳化物及氮化物数量呈现先增长后降低的趋势,在750 ℃时数量最多。而在750 ℃时效5~10 h范围内,随着时效时间的增加,析出相数量变化不大。析出相的析出过程为:先在晶界交叉处析出胞状析出物,随时间的延长,在晶界逐渐析出条状析出物,在晶内开始出现并逐渐长大,最终形成类珠光体的片层状析出。 相似文献
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通过不锈钢在奥氏体区的等温处理,研究不同温度、时间对组织转变的影响.对950℃不同时间等温处理的转变组织作了定量金相分析,并与Dictra软件模拟结果进行比较.结果表明,模拟结果与实验结果符合较好.另外对900℃、1100℃等温以及不同的初始晶粒尺寸进行了模拟,模拟结果显示,900℃、950℃初始阶段主要受相变驱动力因素控制,1100℃合金元素扩散成为控制因素.它们相同的转变全部完成的时间分别为28.9h,6.6h,3.8h.经过模拟计算,晶粒大小对组织转变有较大的影响. 相似文献
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Metal Science and Heat Treatment - 相似文献
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Yusuf Kayg?s?z 《中国铸造》2018,15(5):390-396
The composition of Al-Cu-Mn ternary eutectic alloy was chosen to be Al-32.5 wt.%Cu-0.6 wt.%Mn to the Al2 Cu and Al12 Cu Mn2 solid phases within an aluminum matrix(α-Al) from its melt. The Al-32.5 wt.%Cu-0.6 wt.%Mn alloy was directionally solidified at a constant temperature gradient(G=8.1 K·mm~(-1)) with different growth rates, 8.4 to 166.2 μm·s~(-1),by using a Bridgman-type furnace. The eutectic temperature(the melting point) of 547.85 °C for the Al-32.5 wt.%Cu-0.6 wt.%Mn alloy was obtained from the DTA curve of the temperature difference between the test sample and the inert reference sample versus temperature or time. The lamellar spacings(λ) were measured from transverse sections of the samples. The dependencies of lamellar spacings(λAl-Al2 Cu) and microhardness on growth rates were obtained as, λ_(Al-Al2Cu)=3.02 V~(-0.36), HV=153.2(V)~(0.035), HV=170.6(λ)~(-0.09) and HV=144.3+0.82(λ_(AlAl2 Cu))~(-0.50), HV=149.9+53.48 V~(0.25), respectively, for the Al-Cu-Mn eutectic alloy. The bulk growth rates were determined as λ~2_(Al-Al2 Cu)·V = 25.38 μm~3·s~(-1) by using the measured values of λ_(Al-Al2 Cu) and V. A comparison of present results was also made with the previous similar experimental results. 相似文献
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《International Heat Treatment & Surface Engineering》2013,7(1):6-7
AbstractThe mechanism of decomposition transformation of Fe–N the austenite system has been investigated. An improved process of austenitic nitriding, achieved by applying controlled nitrogen potential theory, allowed high nitrogen austenite samples with a uniform nitrogen concentration to be produced. The key point of this gas nitriding process is to keep the atmosphere at very low nitrogen potential. As a result, the nitride layer on the surface of the pure iron foil was reduced and pure iron ferrite was thoroughly nitrided, forming high N austenite (γ-Fe[N]) that is thermally stable at room temperature. The nitrogen concentration of this austenite was determined as 9·32 at.-%, which is almost the maximum value achievable in Fe–N austenite. 相似文献
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