共查询到18条相似文献,搜索用时 62 毫秒
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新型Mn-Cr齿轮钢的动态再结晶行为研究 总被引:1,自引:0,他引:1
采用Gleeble1500热模拟试验机研究了变形温度、变形速率、变形程度及奥氏体晶粒尺寸对新型Mn-Cr齿轮钢动态再结晶行为的影响。确定了该Mn-Cr齿轮钢的动态再结晶激活能Q及应力指数n分别为378.6kJ/mol和5.81,在热轧齿轮钢管穿孔工序中,变形温度为1100-1150℃,变形量为40%~54%,奥氏体处于动态再结晶状态;而在轧管及减径工序中,变形温度分别为1000~1050℃和900-950℃,变形量分别为21%和31%,奥氏体均处于加工硬化状态。 相似文献
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B30MnSi钢的动态再结晶行为 总被引:4,自引:1,他引:3
采用Gleeble1500热模拟试验机对B30MnSi钢(%:0.32C,1.04Mn,0.85Si,0.019P,0.009S)进行变形温度为850~1000℃,应变速度为0.1~101/s的压缩变形试验,以研究该钢的动态再结晶规律。并通过回归分析得出峰值应力σm,应变εp,动态再结晶临界应变εc与温度补偿变形速率因子Z之间关系式为σm=16.689Ln(Z)-347.41;εp=0.0474Ln(Z)-1.1023;εc≈0.0393Ln(Z)-0.915。 相似文献
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半钢材料的动态再结晶行为 总被引:1,自引:1,他引:0
本文研究了含C1.77%的半钢热变形时奥氏体动态再结晶行为。研究结果表明,在950℃以下进行热变形时,存在一种新的动态再结晶现象:热变形奥氏体不经过形核过程直接碎化为若干个晶粒;其动态再结晶机制是“亚晶界独立生长成为大角度晶界”。在950℃以上或以下的温度范围内,热变形激活能的值也不同;在950℃以上热变形激活能为648.4kJ/mol,在950℃以下热变形激活能为485.1kJ/mol。 相似文献
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采用Gleeble高温压缩实验研究了变形条件对GH625合金高温变形动态再结晶的影响,结果表明:当变形程度较小时,原始晶粒内部出现大量孪晶,晶界呈现锯齿状凸出;随变形程度的增加,在晶界弓出部位开始形核,形成大量再结晶晶粒,随变形程度进一步增加,GH625合金动态再结晶体积分数增大,但是再结晶晶粒尺寸无明显变化;GH625合金动态再结晶是一个受变形温度和应变速率控制的过程,变形温度越高,动态再结晶越容易形核,应变速率越小,动态再结晶过程进行得越充分。在低应变速率条件下,GH625合金获得完全动态再结晶组织的温度随变形速率的升高而升高,而在高应变速率条件下必须考虑变形热效应对合金变形组织的影响。 相似文献
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采用Gleeble-1500D热模拟试验机研究30%SiCp/Al复合材料在温度为623~773 K、应变速率为0.01~10 s-1下的热变形及动态再结晶行为。结果表明:材料的高温流变应力-应变曲线主要以动态再结晶软化机制为特征,峰值应力随变形温度降低或应变速率升高而增大,材料热激活能为272.831 k J/mol。以试验数据为基础,建立q-s和?q/?s-s曲线,从而进一步获得动态再结晶的临界应变和稳态应变,通过试验数据的回归分析,建立动态再结晶的临界应变模型和稳态应变模型,并在此基础上,获得所需要材料的动态再结晶图。 相似文献
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变形温度对ULCB钢动态再结晶的影响 总被引:1,自引:0,他引:1
取得800 MPa级和900 MPa级ULCB钢,在1100~850℃进行单道次变形的热模拟试验,变形量为40%,应变速率为2 s-1。将应力-应变变化特征和显微组织观察相结合,分析研究变形温度对ULCB钢奥氏体动态再结晶的影响规律。结果表明,温度低于950℃时以形变硬化和动态回复为主,奥氏体形变再结晶主要发生在1000℃以上的高温变形中;奥氏体再结晶百分数随变形温度升高而增加,在1050℃变形后奥氏体再结晶百分数约40%,在1100℃变形后则发生完全再结晶。 相似文献
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微合金化钢的多边形铁素体和针状铁素体的细化是获得强韧化和改善冷、热加工工艺性能的重要手段,其性能的获得与热变形态组织结构及再结晶过程有着极其重要的联系。本文试图通过微合金化钢的动态再结晶问题的若干实验结果并就铌对再结晶及热变形组织的影响和控制等问题,从宏观流变曲线及微观机理两方面试作某些理论上的探讨。 相似文献
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Dynamic Recrystallization Behavior in Mn-Cr Gear Steel 总被引:1,自引:0,他引:1
In the deformation process of austenite,the dy-namic recovery and the recrystallization occur,andthe austenite grain changes.First of all,the grainselongate and dislocation densityincreases.The poly-gonization in elongated austenite grain takes placeand the subcrystal forms due to slipping and cli mb-ing of dislocations,i·e·,dynamic recovery(DRV).When the strain reaches a critical value,new grainswill nucleate by bulging of the grain boundaries[1,2].This is so-called dynamic recrystallizat… 相似文献
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《钢铁研究学报(英文版)》2016,(3):238-243
Hot compression experiments conducted on a Gleeble-3500thermo-mechanical simulator and metallographic observation tests were employed to study the critical conditions of dynamic recrystallization(DRX)of 316 LN austenitic stainless steel.The true stress-true strain curves of 316 LN were obtained at deformation temperatures ranging from 900℃to 1 200℃and strain rates ranging from 0.001s-1 to 10s-1.Based on the above tests,the critical conditions of DRX were determined and compared with those obtained from work-hardening theory and the Cingara-McQueen flow stress model.Furthermore,the microstructure was observed to validate the calculated results.The ratio of critical strain to peak strain(εc/εp)for 316 LN was determined,and the quantitative relationship between the critical strain and the deformation parameters of 316 LN was elucidated.The results demonstrated that the onset of DRX corresponds to the constant normalized strain hardening rate(Γ),namely,the critical strain hardening rateΓcfor316LN is equal to 0.65. 相似文献
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Hot compression deformation behaviors of medium carbon Cr-Ni-Mo-Nb steel were investigated at deformation temperatures ranging from 1223 to 1423 Kand strain rates of 0.1,1and 5s-1.Dynamic recovery(DRV)and dynamic recrystallization(DRX)were observed during the hot compression deformation.For all of the samples,DRX occurred at deformation temperatures above 1323 Kat different strain rates,while below 1223 K,no DRX was observed.The activation energy of the tested steel was determined as 386.06kJ/mol.The ratio of critical stress to peak stress and the ratio of critical strain to peak strain were 0.835 and 0.37,respectively.Kinetic equations interpreting the DRX behavior of the tested steel were proposed,and the corresponding parameters including the volume fraction and the average grain size were determined.Moreover,the microstructures induced under different deformation conditions were analyzed. 相似文献
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