研究了球形孔通孔和闭孔泡沫铝合金在1 MHz~10 MHz的超声衰减性能.结果表明:泡沫铝合金的超声衰减性能决定于其孔结构;通孔泡沫铝合金的超声衰减系数α随着孔径d的减小、孔隙率Ps减小和比表面积Sv的增加而增大;闭孔泡沫铝合金的超声衰减系数α随孔径d的减小、孔隙率Ps的增加和比表面积Sv的增加而增大;当孔径d、孔隙率Ps相近时,闭孔泡沫铝合金的超声衰减性能优于通孔泡沫铝合金;在1 MHz~10 MHz二者是具有良好阻尼性能的轻质材料.其衰减机制为在弹性范围内超声应力波在具有大量孔隙界面的泡沫铝合金中的衰减.
参考文献
[1] | M.F.Ashby, A.G.Evans, Metal Foams: A Design Guide, 1st Edition (Boston, B-H Press, 2000)p.23 |
[2] | L.J.Gibson, M.F.Ashby, Cellular Solids, Structures and Properities, Second edition (London, Cambriadge University Press, 1999) p.175 |
[3] | J.Banhart, Norman A.Fleck, Andreas Mortensen, Cellular Metals and Metal Foaming Technology, 1st Edition, (Berlin, Germany, Verlag Metal Innovation Technologie MIT, 2003) p.23 |
[4] | M.F.Ashby, T.J.Lu, Science in China(B), 46(6), 521(2003) |
[5] | YANG Donghui, HE Deping, Science in China (B), 44(4), 411(2001) |
[6] | ZHEN Mingjun, HE Deping, DAI Ge, Science in China(B), 45(18), 598(2002) |
[7] | ZOU Yi, HE Deping, JIANG Jiaqiao, Science in China (B), 47(5), 407(2004) |
[8] | HE Deping, YU Xingquan, Chinese Journal of Materials Research, 11(1), 101(1997)(何德坪,余兴泉,材料研究学报,11(1),101(1997)) |
[9] | LIU Changsong, HAN Fusheng, ZHU Zhengang, Acta Physcia Sinica, 46(8), 1585(1997)(刘长松,韩福生,朱震刚,物理学报,46(8),1585(1997)) |
[10] | J.Banhart, J.Baumeister, M.Weber, Materials Science and Engineering, A205, 221(1996) |
[11] | Richard Weaver, Ultrasonics, 36, 435(1998) |
[12] | Q.Ji, L.H.Le, L.J.Filipow, S.A.Jackson, Ultrasonics, 36, 759(1998) |
[13] | WU Zhaojin, HE Deping, Journal of Applied Sciences, 19(4), 357(2001)(吴照金,何德坪,应用科学学报,19(4),357(2001)) |
[14] | ZHENG Mingjun, HE Deping, Chinese Journal of Material Research, 16(5), 474(2002)(郑明军,何德坪,材料研究学报,16(5),474(2002)) |
[15] | HE Deping, WANG Yongjin, CHEN Ce, YANG Donghui, Preparation of Porous Al Alloy, CN1161486C,2004(何德坪,王永进,陈策,杨东辉,多孔铝合金及其制备方法,CN1161486C,2004) |
[16] | HE Deping, ZHENG Mingjun, Preparation of Closed-Cell Al Alloy Foam, CN1161485C, 2004(何德坪,郑明军,闭孔泡沫铝合金的制备方法,CN1161485C,2004) |
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