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平面流铸法是一种制备非晶和纳米晶薄带的先进技术。这项技术的难点不仅在于快速冷却以抑制薄带的晶化,还在于获得高表面质量的薄带。提出了一种用三维稳态模拟模型预测工业生产中广泛应用的2种单辊冷却结构的流场和传热系数分布的新方法。利用FLUENT软件,结合能量和动量方程,计算了2种结构的流速分布。预测了2种结构的对流换热系数分布。结果表明,水槽结构的速度分布无均匀性,也无周期性;水缝结构的速度分布无均匀性,但具有周期性。2种结构的对流换热系数分布不是中心对称的,水缝结构的冷却特性更为规则。预测了水缝结构的3个对称分布的合适区域,并通过连续生产多次验证。根据热平衡原理,描述了平面流铸法工艺的传热过程。对流换热系数的均匀分布可以作为冷却辊结构设计的依据之一。 相似文献
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Formation and crystallization of Zr-Ni-Ti metallic glass 总被引:1,自引:0,他引:1
The metallic Zr65 Ni25 Ti10 (mole fraction, %) glass has been fabricated by a single roller melt-spinning method. The glass forming ability(GFA) and thermal stability of the Zr65 Ni25 Ti10 melt-spun ribbons were investigated by using X-ray diffraction(XRD) and differential scanning calorimetry(DSC) in the mode of continuous heating. It is shown that the reduced glass transition temperature (Trg) is 0. 506 and the supercooled liquid region (△Tx) is 30 K. Two exothermic peaks were observed in the DSC curves of the as-quenched ribbon, which indicates that the crystallization process undergoes two different stages. The phase transformation during the isothermal annealing was investigated by X-ray diffraction(XRD) and transmission electronic microscope(TEM). It is observed that the metastable FCC Zr2 Ni(Fd3m, a= 12.27 A) precipitated while annealing in the suppercooled region(615 K) and the stable BCT Zr2Ni(I4/mcm, a= 6.499 A, c= 5.270 A) precipitated while annealing at higher temperature(673 K or 723 K). The crystallines are on nanoscale, with grain size of 15-30 nm. The reason for the precipitation of the different structural Zr2 Ni from the glassy matrix under different annealing conditions was discussed based on the concept of multi-component chemical short range order(MCSRO). 相似文献
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钨丝增强ZrTiCuNiBeNb金属玻璃基复合材料界面 总被引:2,自引:1,他引:2
采用渗流铸造工艺制备了钨丝增强ZrTiCuNiBeNb金属玻璃基复合材料,利用X射线衍射、扫描电镜、电子探针以及Nano IndenterⅡ纳米显微力学探针考察了复合材料的界面结构以及界面微区力学性能.结果表明:钨丝增强ZrTiCuNiBeNb金属玻璃基复合材料界面仅由单纯的界面溶解和扩散形成,并未发生界面反应,该界面应属于金属基复合材料的Ⅱ类界面;并且溶解和扩散的存在使界面微区的硬度和弹性模量高于基体,界面结合较强,没有沿界面的裂纹扩展. 相似文献
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金属快速凝固的非平衡超急速传热模型 总被引:2,自引:0,他引:2
运用非Fourier传热理论建立了金属快速凝固过程中的非平衡传热理论模型,包括非Fourier方程的建立、传热与相变模拟,模拟计算表明:(1)在溅射激冷条件下,界面换热系数越大,界面冷却速度和移动速度也越高。在界面换热系数相同时,计算得到的界面冷却速度随着固-液界面高度的提高呈现先上升而后下降的变化趋势;计算得到的冷却速度值明显小于Fourier定律的计算值。(2)在激光加热条件下,计算的界面移动速度在凝固开始时先急剧增加,然后渐趋平稳,计算还表明,金属的过热及过冷度与其热物性相关。 相似文献
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Since the discovery of bulk Zr-Ti-Cu-Ni-Be[1] and Pd-Ni-Cu-P[2] metallic glasses with ex-traordinary high glass forming (GFA) ability and critical cooling rate lower than 100 K/s, great attention has been paid to the structure of BMG alloys. Experimental results of X-ray and neutron diffraction or scattering have provided ample evidence that there is a short-range order in BMG alloys. Metallic glasses always exhibit strong compound forming tendency and the corresponding anomalies of t… 相似文献
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采用瞬态电阻测量方法,对激光表面快速熔凝过程进行了实时跟踪,分析了激光器单脉冲能量、金属薄膜的预热温度等参数对测定结果的影响。结果表明;在快速熔凝过程中金属薄膜的电阻随过程时间呈凸峰状变化,在激光加热周期内,电阻随时间迅速增加,之后随时间的推移又逐渐减小,电阻的减小速度低于增加速度;随着激光功率密度增加,电阻曲线的峰值增大,升温及冷却速度相应增大;随着预热温度的提高,电阻峰值也相应增大,但是样品下表面的热导出率下降,冷却速度下降;当样品下表面的导热能力降低时,样品的电阻曲线峰值有所提高,而在冷却段电阻却明显变化缓慢。 相似文献