共查询到18条相似文献,搜索用时 235 毫秒
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目的研究工艺参数对高温合金Ω截面密封环旋压成形过程的影响规律,解决该类构件旋压成形难题。方法基于ABAQUS/Explicit平台建立了高温合金Ω截面密封环普旋三维有限元模型,通过该模型研究了旋压成形过程中的主要工艺参数对其等效应力、等效塑性应变、壁厚变化的影响规律,进而揭示了各参数对环件成形质量的影响。结果芯模转速增大,不均匀变形程度增大,等效应力峰值先增大后减小,壁厚减薄基本不变;增大旋轮进给率与旋轮圆角半径,均有利于降低不均匀变形程度和等效应力峰值,改善壁厚减薄。结论当芯模转速为10~15rad/s,旋轮进给率为0.8~1.0mm/r,旋轮圆角半径为1.5~2.0 mm时,可以获得成形质量较高的Ω截面密封环。 相似文献
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锥形件变薄旋压回弹的三维有限元分析 总被引:1,自引:0,他引:1
了解锥形件变薄旋压成形后的回弹规律,对提高旋压件的成形质量有重要意义.分别采用动态显式和静态隐式方法建立了锥形件变薄旋压及回弹的三维有限元模型,并研究了芯模转速和旋轮进给比对回弹前后应力、应变及壁厚变化和零件形状的影响.研究表明:随芯模转速增加和旋轮进给比减小,回弹前后最大等效应力差逐渐减小,塑性应变差及壁厚变化基本不变;回弹后最大偏离量随芯模转速和旋轮进给比增大在芯模转速较小时变化不大,而在其较大时随其增大有所减小,并随旋轮进给比增大呈先减小后增大再缓慢减小的趋势. 相似文献
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双辊夹持式板料旋压成形是用来加工薄壁回转体法兰零件的新工艺。为了研究其旋压成形过程中的塑性变形行为,利用ABAQUS软件建立了双辊夹持旋压成形过程的三维有限元模型,并进行了薄壁回转体法兰零件的旋压成形过程的数值模拟,获得了成形过程中等效应力、应变及壁厚的分布。研究了翻边长度对成形件应力应变及壁厚减薄率的影响规律。结果表明等效应力、应变及最大壁厚减薄率均随着翻边长度的增大而增大,由此根据不同的毛坯材料可以确定相应的最大翻边长度。 相似文献
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目的 研究大直径薄壁筒体在对轮强力旋压过程中的应力–应变分布情况和材料流动特征,探明减薄率、进给比和主轴转速等工艺参数对成形结果的影响规律。方法 利用Forge仿真平台建立2.25 m级5052铝合金筒体对轮强力旋压的有限元模型,分析筒体成形过程中的应力–应变状态和主要工艺参数对成形精度与旋压成形力的影响规律。结果 在对轮旋压成形过程中,筒体内外侧应力–应变呈对称分布,成形区域内材料呈扇形流动。工艺参数对成形工件壁厚精度和旋压成形力的影响主次顺序为:减薄率>进给比>主轴转速。结论 各工艺参数的增大均会降低工件的壁厚精度,减薄率和进给比的增大会引起旋压成形力增大,而主轴转速增大会使旋压成形力轻微减小。 相似文献
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变厚度轮辐强力旋压成形过程的分析 总被引:1,自引:0,他引:1
利用ABAQUS/Explicit模拟了变厚度轮辐双道次强力旋压过程,给出了建模和分析结果.轮辐旋压成形伴随板坯的剧烈减薄,收口区域较难成形,减薄率达50%,在计算中,轮辐有限元网格畸变严重,为此运用ALE技术改善网格质量,提高了计算精度.对模拟的旋压轮辐厚度与实验测量值进行了对比,二者吻合较好,验证了计算模型和结果的可靠性.通过ABAQUS/Standard计算了轮辐旋压成形后的回弹变形量和残余应力,分析成形后轮辐等效应变分布及回弹特征,研究发现,回弹变形量与旋压成形时壁厚变化量成正比. 相似文献
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目的 分析Al/Cu双金属管在内旋压增量成形时应力、应变、剪切结合强度的分布情况,研究主要工艺参数对双金属管剪切结合强度的影响规律。方法 基于有限元模拟软件,对Al/Cu双金属管内旋压成形过程进行有限元数值模拟;研究了内旋压增量成形时工艺参数:内管减薄率ψ、两管之间的初始间隙c、旋轮进给比f对剪切结合强度的影响。结果 随着工艺参数内管减薄率ψ、两管之间的初始间隙c、旋轮进给比f的增大,剪切应力数值也随着增大;基管与衬管的高剪切应力值主要集中在旋压结束部分,衬管的长度被拉长,模拟与实验的剪切应力在旋压成形的末端数值明显增大。结论通过有限元数值模拟分析,得出不同的工艺参数对成形质量的影响规律,对实际成形有重要的作用。 相似文献
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工艺参数对剪切旋压旋压力和壁厚差的影响 总被引:3,自引:0,他引:3
在锥形件剪切(变薄)旋压过程中,旋压力分析对于确定工艺参数及设备选型都具有重要意义,而壁厚差是衡量旋压件成形质量的关键指标之一.基于ABAQUS/Explicit平台建立了锥形件剪切旋压的三维有限元模型,进而获得了偏离率、旋轮圆角半径、旋轮进给量、芯模转速及旋轮直径对LY12M锥形件剪切旋压旋压力和壁厚差的影响规律.研究表明:旋压力随偏离率增加而减小,随旋轮圆角半径、旋轮进给量、芯模转速的增加均呈上升变化趋势;偏离正弦律的程度越大,壁厚差越大;旋轮圆角半径为毛坯厚度的1~2倍,壁厚差较小;较大的旋轮进给量和芯模转速有利于减小壁厚差.旋轮直径对旋压力和壁厚差的影响不显著. 相似文献
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C. Häusler H. Jelitto P. Neumeister H. Balke G. A. Schneider 《International Journal of Fracture》2009,155(1):43-54
The elastic stress and strain fields in a plate of finite thickness containing an elliptical hole are systematically investigated
using the 3D finite element method. It is found that the stress and strain concentrations are different in the plate of finite
thickness even if the plate is in an elastic state. The relation between the stress and the strain concentration factors depends
on Poisson’s ratio, the hole’s geometric configuration and the plate thickness. The stress concentration factor is equal to
the strain concentration factor only at the notch root of the plate surface. The stress (or strain) concentration factor at
the notch root of the plate surface decreases rapidly with increasing thickness and becomes lower than the stress and strain
concentration factors corresponding to the plane stress state or at the notch root of the mid plane. It is too low to reflect
the overall stress concentration as the thickness increases or as the b/a ratio decreases. The maximum stress concentration factor occurs on the mid plane only when the plate is thinner than the
transition thickness of the stress concentration factor. When the plate is thicker than the transition thickness of the stress
concentration factor, the distance between the location of the maximum stress concentration factor and plate surface tends
to be constant with increasing thickness for the plate with a given b/a ratio. The differences between the maximum value and the surface value of the stress and strain concentration factors increase
rapidly and tend to their respective constant values with increasing plate thickness. The smaller the b/a ratio, the larger these differences. The difference of the stress concentration factor is larger than that of the strain
concentration factor in the same plate. 相似文献
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工艺参数对AZ31镁合金往复挤压过程的影响 总被引:1,自引:0,他引:1
运用刚黏塑性有限元法对不同工艺参数下的AZ31镁合金往复挤压过程进行了热力耦合数值模拟,研究了不同初始坯料温度、挤压速率和摩擦因数对往复挤压过程中等效应变、等效应力及温度场的影响。结果表明:在往复挤压过程中,挤压速率对等效应变峰值影响不大,随着挤压速率的增大,工件内温度峰值直线上升,温度分布不均匀程度增大,应力峰值先增加后减小;随着初始坯料温度升高,等效应力峰值呈直线趋势减小;摩擦因数对温度峰值的影响很小,随着摩擦因数的增大,等效应变峰值先增大然后趋于平稳,等效应力峰值增大,其增大幅度减小。 相似文献
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运用有限元仿真软件ABAQUS对体积分数为56%的SiCp/Al复合材料薄壁回转体在静载荷作用下的应力、变形及应变进行了仿真研究,研究了载荷施加位置、外径和壁厚对SiCp/Al复合材料圆筒薄壁件的应力、变形及应变的影响规律。结果表明:在其他条件一致的情况下,回转体的外径越小、壁厚越大、受力点距离施加全约束的一端越近,回转体受到外载荷引起的最大应力、最大变形及最大应变越小。薄壁回转体工件的壁厚对工件最大应力、最大变形及最大应变的影响最为显著。当壁厚增加到1mm以上时,最大应力、最大变形及最大应变的变化不明显。 相似文献
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Haitao ZHOU Liufa LIU Qudong WANG Da LU Xiaoqin ZENG Wenjiang DINGNational Engineering Research Center of Light Alloys Net Forming School of Materials Science Engineering Shanghai Jiao Tong University Shanghai China 《材料科学技术学报》2004,20(6):691-693
The deformation behavior of AZ61 Mg alloy during hot deformation has been investigated in wide temperature and strain rate range by a Gleeble simulator. Specimens are deformed in compression in the temperature range of 523~673 K and at strain rates of 0.001~1 s-1. It is found that the flow curves exhibit a peak and then decrease towards steady-state of classical DRX, which decrease with rising temperature and decreasing strain rate. The deformation behavior of the specimens can be attributed to the occurrence of strain hardening and softening. As stress decreases, the strain hardening rate declines at a fast rate when temperature rises or strain rate decreases. The shapes of θ-σ curves indicate some important features such as subgrain formation, the critical stress, the peak stress and steady stress. The onset of DRX can be determined by the point of inflection on θ-σ or Inθ-σ curves. 相似文献
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The hot compressive deformation behavior of a new hot isostatically pressed Ni–Cr–Co based powder metallurgy (P/M) superalloy was studied in the temperature range of 950–1150 °C and strain rate range of 0.0003–1 s−1 using Gleeble-1500 thermal simulator. The dynamic recrystallization-time–temperature (RTT) curve was developed and the constitutive equation of flow stress during hot deformation was established. The results show that the flow stress decreases with increasing deformation temperature and decreasing strain rate. The flow stress represents as the characteristic of dynamic crystallization with the increasing of strain at the deformation temperatures lower than 1100 °C and strain rates higher than 0.0003 s−1. The beginning time of dynamic crystallization has no linear relationship with deformation temperature in the condition of strain rate lower than 0.01 s−1. Besides, the experiments verify that the hyperbolic sine model including the variable of strain reflects the changing law of flow stress during the hot deformation process. 相似文献
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利用Gleeble-3500热模拟试验机对Mg-9Al-3Si-0.375Sr-0.78Y合金试样进行等温恒应变速率压缩实验,研究其在温度250~400℃、应变速率0.001~10s~(-1)条件下的热变形行为。结果表明:在热变形过程中,峰值应力随着应变速率的降低和温度的升高而减小,且峰值应力对应变速率的敏感性随着变形温度的下降而增强。建立了考虑应变的热变形Arrhenius本构模型,模型精度良好,在300,350℃及0.001~10s~(-1)范围内,模型的平均绝对误差分别为1.57%和1.76%;合金的平均变形激活能为183.58k J/mol,平均应变速率敏感指数为0.1616。热变形过程中,α-Mg相呈现明显的动态再结晶特征,β-Mg17Al12相尺寸减小且分布均匀,初生Mg_2Si相较小。在低温(250~300℃)变形时,动态再结晶仅发生在晶界处。在高温(350~400℃)变形时,初生α-Mg晶粒发生了明显的动态再结晶。随着温度的增加和应变速率的降低,再结晶程度提高,再结晶晶粒逐渐长大。 相似文献