欢迎登录材料期刊网

材料期刊网

高级检索

在对填料颗粒堆积简化的基础上,建立了由渗流单元组成的二维微管模型.使用该模型对渗流过程进行模拟计算,渗流时间的计算值与实验值符合良好,并获得渗流过程的如下新规律:铝熔体在流过填料颗粒时,在填料颗粒的背压区封闭一定质量的气体,封闭的气体使附加孔隙率和通孔度增大.在渗流过程中静压力的变化分两个阶段:渗流开始时,静压力先缓慢增加,在渗流结束时瞬间,压力增加到最大值;后者对高孔隙率多孔铝的制备有重要意义.这些渗流规律为控制渗流过程和孔结构提供了依据.

参考文献

[1] Lorna J.Gibson,Michael F.Ashby.Cellular SolidsStructure and Properties,Second Edition,(Cambridge University Press,1997) p.17
[2] M.F.Ashby,A.G.Evans,Metal Foams:A Design Guid.,1st Edition (Boston,B-H press,2000) p.23
[3] John Banhart.Progress in Materials Science,46,559(2001)
[4] HE Deping,WEN Desun,ZHANG Yong,Sbu Guangji,Journal of Materals Research,11(2),113(1997)(何德坪,闻德荪,张勇,舒光冀,材料研究学报,11(2),113(1997))
[5] CHENG Guiping,CHENG Hongden,WEN Desun,SHU Guangji,The Chinese Journal of Nonferrous Metal,10(1),85(2000)(程桂萍,陈宏灯,闻德荪,舒光冀,中国有色金属学报,10(1),85(2000))
[6] A.Mortensen,L.J.Masurl,J.A.Cornie,M.C.Flemings,Metall.Trans.,20A(11),2535(1989)
[7] H.Ristow,Pattern Formation in Granular Materials,Springer-Verlag,Berlin,Heidelberg (2000)
[8] Viktor K.Horvath,Imre M.Janosi,Peter J.Vella,Phys.Rev.E.54,1996(2005)
[9] L.Vanel,E.Clement,Eur.Phys.,11(1B),525(1999)
[10] WANG Xianfu,XIONG Aokui,Advanced Fluid Dynamics,(WuHan,HUST Publishing Comp,2003) p.3(王献孚,熊鳌魁,高等流体力学,武汉,华中科技大学出版社.2003(P3))
[11] Nichols B.D.,Hirt C.W.,Hotchliss R.S.,SOLA-VOF:a solution algorithm for transient fluid flow with multiple free boundaries.Tech Report LA-8355,Los Alamos Scientific Laboratory,1980
[12] LI Wanping,Computational Fluid Dynamics,(WuHan,HUST Publishing Comp,2004) p.35(李万平,计算流体力学,(武汉,华中科技大学出版社,2004)p.35)
[13] V.Yakhot,S.A.Orzag,Renormalization group analysis of turbulence:basic theory.J.Scient.Comput.,1:3-11,1986
[14] CHENG Guiping,Preparing Porous Al and Rsearch of Metal Infiltration,PhD Dissertation,Nanjing,Southeast University,1997(程桂萍,多孔铝的制备及液态金属渗流动力学的研究,东南大学:材料科学与工程系,1997)
[15] HE Deping,ZHANG Weikai,LI Naizhe,China patent,CN.2004100155.7,1(2004)(何德坪,张伟开,李乃哲,CN.2004100155.7,1(2004))
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%