References:
[1] Haynes alloy 188, Report-Haynes International, Inc., Kokomo, TN, 1991.
[2] G. R. Halford, J. F. Saltsman, S. Kalluri, " High Temperature Fatigue Behaviour of Haynes 188,”edited by R. J. Richmond and S. T. Wu., Proc. Advanced Earth-to-Orbit Propulsion Technology Conf., MSFC, Huntsville, AL, NASA CP-3012, NASA, Washington, DC, 18-988, May 10-13, 1988, pp. 497-507.
[3] S. Y. Lee, Y. L. Lu, P. K. Liaw, H. Choo, S. A. Thompson, J. W. Blust, P. F. Browning, A. K. Bhattacharaya, J. M. Aurrecoechea and D. L. Klarstrom, "High-temperature tensile-hold crack-growth behaviorof HASTELLOY® X alloy compared to HAYNES® 188and HAYNES® 230® alloys,” Mech. Time-Depend. Mate. 12, 31-44 (2008).
[4] P. J. Bonacuse and S. Kalluri,”Elevated Temperature Axial and Torsional Fatigue Behavior of Haynes 188,”J. Eng. Mater. Tech. 117, 191-199 (1995).
[5] S. Nemat-Nasser, Y. F. Li, J.B. Isaacs,”Experimental/ computational evaluation of flow stress at high strain rates with application to adiabatic shear banding,” Mech. Mater. 17,111-134(1994).
[6] M.A. Meyers, Y.J. Chen, F.D.S.Marguis and D.S. Kim,” High-strain, high strain-rate behavior of tantalum” Metall. Mater. Trans. A26, 2493-2501 (1995).
[7] A. G. Odeshi and M. N. Bassim,"High strain-rate fracture and failure of a high strength low alloy steel in compression," Mater. Sci. Eng. A 525, 96-101(2009).
[8] WR. C. Batra and D. Liu,"Adiabaticshear banding in plane strain problems," ASME J. Appl. Mech. 56, 527-534(1989).
[9] L. E. Murr, A. C. Ramirez, S. M. Gaytan,M. I. Lopez,E. Y. Martinez,D. H. Hernandez and E. Martinez, "Microstructure evolution associated with adiabatic shear bands and shear band failure in ballistic plug formation in Ti–6Al–4V targets,” Mater. Sci. Eng. A 516, 205-216(2009).
[10] U.S. Lindholm,” Some experiments with the split hopkinson pressure bar∗,” J. Mech. Phys. Sol. 12, 317-335 (1964).
[11] W. S. Lee and C. F. Lin,”Plastic deformation and fracture behaviour of Ti–6Al–4V alloy loaded with high strain rate under various temperatures,” Mater. Sci. Eng. A. 241,48-59(1998).
[12] P. S. Follansbee and U. F. Kocks,” A constitutive description of the deformation of copper based on the use of the mechanical threshold stress as an internal state variable,”Acta Metall. 36, 81-93(1988).
[13] W. G. Guo and S. Nemat-Nasser,”Flow stress of Nitronic-50 stainless steel over a wide range of strain rates and temperatures.”Mech. Mater. 38, 1090-1103 (2006).
[14] J. Litonski,” Plastic Flow of a Tube Under Adiabatic Torsion,” Bull. Acad. Pol. Sci. Ser. Sci. Technol. 25, 7–14(1977).
[15] F. J. Zerilli and R. W. Armstrong,” Dislocation-mechanics based constitutive relations for material dynamics calculations,"J. Appl. Phys.61(5), 1816-1825 (1987).
[16] S. R. Bodner, and Y. Partom,” Constitutive equations for elastic strain-hardening meterials,”J. Appl. Mech. 385-389(1975).
[17] A. S. Khan, Y. S. Suh and R. Kazmi,” Quasi-static and dynamic loading responses and constitutive modeling of titanium alloys,”Int. J. Plasticity 20, 2233-2248(2004).