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Spall strength and Hugoniot elastic limit of a zirconium-based bulk metallic glass under planar shock compression

Published online by Cambridge University Press:  03 March 2011

Fuping Yuan
Affiliation:
Case School of Engineering, Department of Mechanical and Aerospace Engineering, Case Western Reserve University, Cleveland, Ohio 44106-7222
Vikas Prakash*
Affiliation:
Case School of Engineering, Department of Mechanical and Aerospace Engineering, Case Western Reserve University, Cleveland, Ohio 44106-7222
John J. Lewandowski*
Affiliation:
Case School of Engineering, Department of Materials Science and Engineering, Case Western Reserve University, Cleveland, Ohio 44106-7222
*
a) Address all correspondence to this author. e-mail: [email protected]
b)This author was an editor of this focus issue during the review and decision stage. For the JMR policy on review and publication of manuscripts authored by editors, please refer to http://www.mrs.org/jmr_policy.
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Abstract

Results are presented on the shock response of a zirconium-based bulk metallic glass (BMG), Zr41.25Ti13.75Ni10Cu12.5Be22.5, subjected to planar impact loading. An 82.5-mm bore single-stage gas-gun facility at Case Western Reserve University, Cleveland, OH, was used to conduct the shock experiments. The particle velocity profiles, measured at the back (free) surface of the target plate by using the velocity interferometer system for any reflector (VISAR), were analyzed to (i) better understand the structure of shock waves in BMG subjected to planar shock compression, (ii) estimate residual spall strength of the BMG after different levels of shock compression, and (iii) obtain the Hugoniot elastic limit (HEL) of the material. The spall strength was found to decrease moderately with increasing levels of the applied normal impact stress. The spall strength at a shock-induced stress of 4.4 GPa was 3.5 GPa while the spall strengths at shock-induced stresses of 5.1, 6.0, and 7.0 GPa were 2.72, 2.35, and 2.33 GPa, respectively. The HEL was estimated to be 6.15 GPa.

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Articles
Copyright
Copyright © Materials Research Society 2007

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References

REFERENCES

1Bruck, H.A., Rosakis, A.J., and Johnson, W.L.: The dynamic compressive behavior of beryllium bearing bulk metallic glasses. J. Mater. Res. 11, 503 (1996).CrossRefGoogle Scholar
2Lewandowski, J.J. and Lowhaphandu, P.: Effects of hydrostatic pressure on mechanical behavior and deformation processing of materials. Int. Mater. Rev. 43, 145 (1998).CrossRefGoogle Scholar
3Inoue, A. and Hashimoto, K.: Amorphous and Nanocrystalline Materials: Preparation, Properties and Applications (Springer-Verlag, Berlin, Germany, 2001).CrossRefGoogle Scholar
4Peker, A. and Johnson, W.L.: A highly processable metallic glass—Zr41.2Ti13.8Cu12.5Ni10.0Be22.5. Appl. Phys. Lett. 63, 2342 (1993).CrossRefGoogle Scholar
5Johnson, W.L.: Bulk Metallic Glasses edited by Johnson, W.L., Inoue, A. and Liu, C.T. (Mater. Res. Soc. Symp. Proc. 554, Warrendale, PA, 1999), pp. 311339.Google Scholar
6Lu, J.: Mechanical behavior of a bulk metallic glass and its composites over a wide range of strain rates and temperatures. Ph.D. Dissertation, California Institute of Technology, Pasadena, CA (2002).Google Scholar
7Hufnagel, T.C., Jiao, T., Li, Y., Xing, L.Q., and Ramesh, K.T.: Deformation and failure of Zr57Ti5Cu20Ni8Al10 bulk metallic glass under quasi-static and dynamic compression. J. Mater. Res. 17, 1441 (2002).CrossRefGoogle Scholar
8Subhash, G., Zhang, H., and Li, H.: Thermodynamic and mechanical behavior of hafnium/zirconium based bulk metallic glasses, in Proceedings of the International Conference of Mechanical Behavior of Materials (ICM-9) (Kenes International, Geneva, Switzerland, 2003), p. 1A5.Google Scholar
9Sunny, G.P., Lewandowski, J.J., and Prakash, V.: Dynamic compression of amorphous and annealed bulk metallic glass, in Proceedings of the 2006 SEM Annual Conference and Exposition on Experimental and Applied Mechanics St. Louis, MO (Society of Experimental Mechanics, Bethel, CT, 2006), Paper # 349.Google Scholar
10Sunny, G.P., Prakash, V., and Lewandowski, J.J.: Effects of annealing on dynamic behavior of a bulk metallic glass, in Proceedings of the 2005 International Mechanical Engineering Conference and Exposition, ASME (American Society of Mechanical Engineers, New York, 2005), Paper # IMECE2005-83016.Google Scholar
11Sunny, G.P., Prakash, V., and Lewandowski, J.J.: Results from a novel insert design for high starin-rate compression of a bulk metallic glass, in Proceedings of the 2006 International Mechanical Engineering Conference and Exposition, ASME (American Society of Mechanical Engineers, New York, 2006), Paper # IMECE2006-15414.Google Scholar
12Sunny, G.P., Yuan, F., Lewandowski, J.J., and Prakash, V.: Dynamic stress-strain response of a Zr-based bulk metallic glass, in Proceedings of the 2005 SEM Annual Conference and Exposition on Experimental and Applied Mechanics (Society of Experimental Mechanics, Bethel, CT, 2005), Paper # 324.Google Scholar
13Bach, J., Krueger, B., and Fultz, B.: Shock wave consolidation of a Ni–Cr–Si–B metallic-glass powder. Mater. Lett. 11, 383 (1991).CrossRefGoogle Scholar
14Conner, R.D., Dandliker, R.B., Scruggs, V., and Johnson, W.L.: Dynamic deformation behavior of tungsten-fiber/metallic-glass matrix composites. Int. J. Impact Eng. 24, 435 (2000).Google Scholar
15Zhuang, S.M., Lu, J., and Ravichandran, G.: Shock wave response of a zirconium-based bulk metallic glass and its composite. Appl. Phys. Lett. 80, 4522 (2002).Google Scholar
16Hays, C.C., Kim, C.P., and Johnson, W.L.: Microstructure controlled shear band formation and enhanced plasticity of bulk metallic glasses containing in situ formed ductile phase dendrite dispersions. Phys. Rev. Lett. 84, 2901 (2000).Google Scholar
17Turneaure, S.J., Winey, J.M., and Gupta, Y.M.: Compressive shock wave response of a Zr-based bulk amorphous alloy. Appl. Phys. Lett. 84, 1692 (2004).Google Scholar
18Yang, C., Liu, R.P., Zhang, B.Q., Wang, Q., Zhan, Z.J., Sun, L.L., Zhang, J., and Gong, Z.Z.: Void formation and cracking of Zr41Ti14Cu12.5–Ni10Be22.5 bulk metallic glass under planar shock compression. J. Mater. Sci. 40, 3917 (2005).CrossRefGoogle Scholar
19Yang, C., Wang, W.K., Liu, R.P., Zhang, X.Y., and Li, X.: Damage features of Zr41Ti14Cu12.5Ni10Be22.5 bulk metallic glass impacted by hypervelocity projectiles. J. Spacecr. Rockets 43, 565 (2006).Google Scholar
20Mashimo, T., Togo, H., Zhang, Y., Uemura, Y., and Kawamura, Y.: Shock-compression behavior of Zr-based metallic glass, in 12th International Symposium on Plasticity and its Applications: Anisotropy, Texture, Dislocations and Multiscale Modeling in Finite Plasticity and Viscoplasticity and Metal Forming, edited by Khan, A.S. and Kazmi, R. (Neat, Inc., Fulton, MD, 2006), pp. 157159.Google Scholar
21Lowhaphandu, P. and Lewandowski, J.J.: Fracture toughness and notched toughness of bulk amorphous alloy: Zr–Ti–Ni–Cu–Be. Scripta Mater. 38, 1811 (1998).CrossRefGoogle Scholar
22Kim, K.S., Clifton, R.J., and Kumar, P.: A combined normal and transverse displacement interferometer with an application to impact of Y-cut quartz. J. Appl. Phys. 48, 4132 (1977).CrossRefGoogle Scholar
23Barker, L.M. and Hollenbach, R.E.: Laser interferometer for measuring high velocities of any reflecting surface. J. Appl. Phys. 43, 4669 (1972).CrossRefGoogle Scholar
24Prakash, V.: A pressure-shear plate impact experiment for investigating transient friction. Exp. Mech. 35, 329 (1995).CrossRefGoogle Scholar
25Grady, D.E. and Kipp, M.E.: High-Pressure Shock Compression of Solids (Springer-Verlag, Berlin, Germany, 1993).Google Scholar
26Mashimo, T.: Effect of shock compression on ceramic materials, in High-Pressure Shock Compression of Solids III, edited by Davison, L. and Shahinpoor, H. (Springer-Verlag, New York, 1998), pp. 101146.Google Scholar
27Fowles, G.R.: Shock wave compression of hardened and annealed 2024 Aluminum. J. Appl. Phys. 32, 1475 (1961).CrossRefGoogle Scholar
28Lewandowski, J.J. and Lowhaphandu, P.: Effects of hydrostatic pressure on the flow and fracture of a bulk amorphous metal. Philos. Mag. A82, 3427 (2002).CrossRefGoogle Scholar
29Espinosa, H.D., Xu, Y., and Brar, N.S.: Micromechanics of failure waves in glass: I. Experiments. J. Am. Ceram. Soc. 80, 2061 (1997).CrossRefGoogle Scholar
30Cagnoux, J. and Longy, F.: Spallation and shock-wave behavior of some ceramics. J. Phys. Coll. 49, 3 (1988).Google Scholar
31Shazly, M.: Dynamic deformation and failure of gamma-Met PX at room and elevated temperatures. Ph.D. Dissertation, Case Western Reserve University, Cleveland, OH (2005).Google Scholar
32Bartkowski, P.T. and Dandekar, D.P.: Spall strengths of sintered and hot pressed silicon carbide, in Shock Compression of Condensed Matter—1995, edited by Schmidt, S.C. and Tao, W.C. (American Institute of Physics, New York, 1996), pp. 535539.Google Scholar
33Dandekar, D.P.: Spall strength of silicon carbide under normal and simultaneous compression-shear shock wave loading. Int. J. Appl. Ceram. Technol. 1, 261 (2004).CrossRefGoogle Scholar
34Nathenson, D.I., Prakash, V., and Dandekar, D.P.: Dynamic response of silicon nitride under combined pressure and shear impact, in Proceedings of the 2005 SEM Annual Conference and Exposition on Experimental and Applied Mechanics (Society of Experimental Mechanics, Bethel, CT, 2005), Paper # 315 (s22).Google Scholar
35Tsai, L. and Prakash, V.: Dynamic response and spall strength of S2-glass fiber reinforced polymer composites, in Proceedings of the 2005 SEM Annual Conference and Exposition on Experimental and Applied Mechanics (Society of Experimental Mechanics, Bethel, CT, 2005), Paper # 322 (s57).Google Scholar