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材料研究学报  2014, Vol. 28 Issue (6): 476-480    DOI: 10.11901/1005.3093.2013.764
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凝固速率对藕状多孔金属结构的影响
李雨耕,金青林(),杨天武,李再久
昆明理工大学材料科学与工程学院 昆明 650000
Influence of Solidification Rate on Pore Structure of Lotus-type Porous Metals
Yugeng LI,Qinglin JIN(),Tianwu YANG,Zaijiu LI
School of Material Science and Engineering Kunming University of Sciences and Technology, Kunming 650000
引用本文:

李雨耕,金青林,杨天武,李再久. 凝固速率对藕状多孔金属结构的影响[J]. 材料研究学报, 2014, 28(6): 476-480.
Yugeng LI, Qinglin JIN, Tianwu YANG, Zaijiu LI. Influence of Solidification Rate on Pore Structure of Lotus-type Porous Metals[J]. Chinese Journal of Materials Research, 2014, 28(6): 476-480.

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摘要: 

使用自制的Gasar装置制备出Cu、Mg和Ni三种藕状多孔金属, 将理论计算与实验结果相结合研究了材料的凝固速率对多孔结构的影响。结果表明, 对于三种多孔金属, 随着气泡半径的增大气泡的上浮速率逐渐增大。仅当金属凝固速率最大值在气泡上浮速率的范围内, 才能制备出有大量规则气孔的藕状多孔结构。

关键词 金属材料Gasar藕状多孔金属定向凝固凝固速率气孔结构    
Abstract

Lotus-type porous Cu, Mg and Ni were fabricated by a mould casting technique in hydrogen gas atmosphere. The effect of solidification rate on the structure of the lotus type porous metals was comparatively investigated by theoretical calculation and experiments. The results show that the increase of bubble radius results in an increase of bubble rising velocity for Cu, Mg and Ni. A suitable ordered porous structure can be obtained only when the maximum solidification rate is in the range of bubble rising velocity.

Key wordsmetallic materials    Gasar    lotus-type metals    unidirectional solidification    solidification rate    pore structure
收稿日期: 2013-10-16     
图1  定向凝固时气泡逸出示意图
图2  理想多孔藕状结构示意图
Physical quantity Symbol (unit) Cu Mg Ni
Melting point Tm(K) 1356 922 1756
Cooling temperature T0(K) 298 373 298
Interfacial energy slg[16](J/m2) 1.31 0.57 1.75
Solute distribution constant k 0.35[17] 0.69[17] 0.41[18]
Diffusion coefficient D H [19] (mm2/s) D H C u =0.512exp (-24600/RTm) D H M g =0.87exp (-29820/RTm) D H N i =0.77exp (-7436/RTm)
Viscosity η[20] (mPas) 4.0 1.25 4.5
表1  计算中用到的材料的热物性参数
图3  高压定向凝固装置示意图
Sample No. Material porosity ε(%) Sample height S(m)
1 Cu 53.6 0.18
2 Mg 44 0.14
3 Ni 10 0.5
表2  实验结果
图4  试样Cu、Mg和Ni的横、纵截面
图5  由stokes公式算出的Cu、Mg和Ni气泡上浮速率与气泡半径的关系以及r和基体凝固速率最大值
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