Texture evolution and anisotropy in the thermo-mechanical response of UFG Ti processed via equal channel angular pressing
Highlights
► Equal channel angular pressing was performed on grade 1 titanium for four passes. ► The initial, uniform microstructure forms mostly ultrafine grains after four passes. ► The yield strength and flow stress were different in the different loading directions. ► Dynamically loaded specimens experienced shear band failure. ► The yield strength in tension was always higher than in compression.
Introduction
Equal channel angular pressing (ECAP) is a technique using severe plastic deformation to produce ultrafine grain (UFG) sizes in the range of hundreds of nanometers to bulk course grained materials (Segal et al., 1981, Valiev et al., 1993, Segal, 1995, Furukawa et al., 1998). ECAP is performed by pressing a billet of material through a die that has two channels which intersect at an angle. The billet experiences simple shear deformation, at the intersection, without any precipitous change in the cross sectional area because the die does not allow for lateral expansion. A single pass with channels 90° to each other, induces approximately 1.15 equivalent strain in the billet, so the billet can be pressed more than once.
Titanium subjected to a single pass of ECAP showed twinning as the dominant deformation mechanism (Kim et al., 2001, Kim et al., 2003, Alexandrov et al., 2008). After two passes, Shin et al. (2003) concluded for route B the dominant mechanism was type a slip. There are several papers that report on the texture of titanium after ECAP, but data are only given in one state – after a single pass (Shin et al., 2003), during pass 3/4 (Chen et al., 2010), and eight passes (Alexandrov et al., 2004, Gubicza et al., 2003). Finally, Suwas et al. (2011) reports on the texture as a function of the number of passes (up to three) and for different processing routes.
For ECAP Ti, Zhernakov et al. (2001) notes that route BC results in higher strength and ductility, another study by Stolyarov et al. (2001) reported that route BC is most effective at producing equiaxed grains and reducing their size. Tabachnikova et al. (2005) reported that the strength in compression is noticeably greater than tension down to 4.2 K. Anisotropy in the mechanical behavior and texture of coarse grained pure titanium is well known (Nixon et al., 2010a, Nixon et al., 2010b), but only a couple of papers have reported on the anisotropy of titanium following ECAP (Korshunov et al., 2008, Sabirov et al., 2011). Korshunov et al. found that for two different shipments the yield strength from highest to lowest was in general in the z, y, and x loading directions (see Fig. 1), respectively, for up to four passes and at both 22 and 450 °C testing temperatures.
Two studies on CP Ti processed by ECAP warrant a review since they perform experiments at dynamic strain rates. The first by Jia et al. (2001), ECAP is done at 450 °C and for eight passes, and compression experiments are performed at room temperature. The UFG Ti is essentially perfectly plastic for both quasi-static and dynamic strain rates, and only the dynamic specimens fail. Later Wang et al. (2007) prepared UFG Ti similarly to Jia et al. but received different flow stresses. The UFG Ti, at quasi-static strain rates, showed perfectly plastic behavior until about 12% true strain when the strain hardening increased, with failure at about 35%. In the dynamic regime, the work hardening is positive from the beginning of the flow stress, but at about 12%, the work hardening greatly increases, and failure occurs at about 23%. A number of high strain rate experiments on UFG and nanocrystalline materials subjected to different processing methods, in addition to ECAP, have been performed by Gray et al., 1997, Jia et al., 2001, Khan and Meredith, 2010, Farrokh and Khan, 2009, among others.
In this study, grade 1 titanium specimens were processed by ECAP for up to four passes at 275 °C, using route BC. The microstructure was observed (optically) without ECAP and at one, two, three and four passes, and the crystallographic texture was examined to determine the evolution due to the ECAP process. Next, the temperature and strain rate (quasi-static to dynamic) sensitivities of the material under uniaxial compressive loadings were investigated to elucidate their changes in different sample loading directions, and the dynamic failure of the material was explored. Finally, the tension/compression asymmetry is presented.
Section snippets
Material
The material subjected to the ECAP process was grade 1 titanium, with the impurity levels given in Table 1. The specimens were obtained from a plate that was cut into strips such that the lengths of the strips were parallel to the rolling direction of the plate.
Equal channel angular pressing procedures
The billets were 12.7 mm in diameter and 82.5 mm in length. The ECAP die had a channel angle of 90° and a corner angle of approximately 20°. For these dimensions, the equivalent strain for each pass subjected to each specimen is about 1.
Microstructural analysis and texture evolution
Fig. 2a is an optical micrograph of the as-received Ti, with the rolling and normal directions oriented horizontally and vertically, respectively. The RD-ND plane is displayed because the shear direction during the first pass of ECAP will be approximately 45° counterclockwise from the rolling direction, as indicated by the pair of arrows. The indicated shear direction (SD) is for the billet exiting the die from right to left, which is shown in Fig. 1b. The microstructure appears deformation
Conclusions
In this study, the texture evolution and anisotropy in the thermo-mechanical behavior of grade 1 titanium subjected to the ECAP process, was investigated at many different temperatures and strain rates. ECAP was performed at 275 °C for up to four passes, which is at a lower temperature than what others have done. The uniform microstructure from the as-received condition, goes from long, coarse bands with some grains relatively undeformed after a single pass to mostly uniform fine and ultrafine
Acknowledgements
This work was supported by the GAANN fellowship from the Department of Mechanical Engineering at UMBC. Brady Butler at the Army Research Lab, in Aberdeen, MD performed the XRD experiments. The salt used for heating the billets was obtained free of charge from Hubbard-Hall Inc.
References (38)
- et al.
Analysis of deformation behavior of Ti in different structural states
Mater. Sci. Eng. A
(2008) - et al.
Ideal orientations and persistence characteristics of hexagonal close packed crystals in simple shear
Acta Mater.
(2007) - et al.
Analysis of texture evolution in magnesium during equal channel angular extrusion
Acta Mater.
(2008) - et al.
Microstructure evolution of commercial pure titanium during equal channel angular pressing
Mater. Sci. Eng.
(2010) - et al.
Microstructure and mechanical properties of microalloyed and equal channel angular extruded Mg alloys
Scripta Mater.
(2008) - et al.
Grain size, strain rate, and temperature dependence of flow stress in ultra-fine grained and nanocrystalline Cu and Al: synthesis, experiment, and constitutive modeling
Int. J. Plasticity
(2009) - et al.
The shearing characteristics associated with equal-channel angular pressing
Mater. Sci. Eng.
(1998) - et al.
Influence of strain rate & temperature on the mechanical response of ultrafine-grained Cu, Ni, and Al–4Cu–0.5Zr
Nanostruct. Mater.
(1997) - et al.
Thermo-mechanical response of Al 6061 with and without equal channel angular pressing (ECAP)
Int. J. Plasticity
(2010) - et al.
Mechanically alloyed nanocrystalline iron and copper mixture: behavior and constitutive modeling over a wide range of strain rates
Int. J. Plasticity
(2000)
Quasi-static and dynamic loading responses and constitutive modeling of titanium alloys
Int. J. Plasticity
Effect of oxygen content and microstructure on the thermo-mechanical response of three Ti-6Al-4V alloys: Experiments and modeling over a wide range of strain-rates and temperatures
Int. J. Plasticity
Effects of equal channel angular pressing temperature on the deformation structures of pure Ti
Mater. Sci. Eng.
Effects of the number of equal-channel angular pressing passes on the anisotropy of ultra-fine titanium
Mater. Sci. Eng.
The influence of ECAP temperature on the stability of Al–Zn–Mg–Cu alloy
J. Alloys Compds
Development of a multi-pass facility for equal-channel angular pressing to high total strains
Mater. Sci. Eng.
Anisotropic response of high-purity α-titanium: experimental characterization and constitutive modeling
Int. J. Plasticity
Experimental and finite-element analysis of the anisotropic response of high-purity α-titanium in bending
Acta Mater.
Anisotropy of mechanical properties in high-strength ultra-fine-grained pure Ti processed via a complex severe plastic deformation route
Scripta Mater.
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