Effect of grain size on the activation energy for plastic deformation near room temperature in a Zn–28.7 pct Al–1.9 pct Cu alloy
Effect of grain size on the activation energy for plastic deformation near room temperature in a Zn–28.7 pct Al–1.9 pct Cu alloy
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DOI:
10.1007/s10853-007-1751-2
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发表时间:
2007-06
影响因子:
4.5
通讯作者:
J. Muñoz‐Andrade;A. Mendoza-Allende;E. Cabrera;G. Torres-Villaseñor;J. Montemayor-Aldrete
中科院分区:
文献类型:
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作者:
J. Muñoz‐Andrade;A. Mendoza-Allende;E. Cabrera;G. Torres-Villaseñor;J. Montemayor-Aldrete
The Zn–22 wt pct Al eutectoid alloy is a superplastic material which has been used in a number of experimental investigations of superplasticity. Considerable attention has been devoted to this alloy, because this material has numerous potential applications [1]. Zinc-rich aluminum alloys with: Fe [2, 3] or with Copper additions [2–5], has been of engineering interest over recent years, because the addition of some alloying elements enhances the wear resistance, elastic modulus, yield strength and corrosion resistance under the service conditions of stress and temperature without having a major effect on the superplastic behavior during production of components. The main goal of this investigation is to study the effect of grain size on the activation energy for plastic deformation, near room temperature, in a Zn–Al–Cu Alloy. The chemical analysis of the alloy used in this work was Zn–28.7 wt pct Al–1.9 wt pct Cu. The superplastic material was obtained by extrusion resulting in a grain size 2.7 μm. A number of flat tensile specimens were prepared from this material. A set of specimens were heat treated at 548 K for 3h, followed by rapid quenching in water at room tempeature. This treatment produce a grain size of 0.6 μm, measured by the line intercept method [6]. The experiments were conducted using two grain size specimens. Flat tensile specimens, having 1.6 cm gage length and 0.2× 0.32 cm cross-section, were used to study creep behavior. Creep tests were carried out using a constant load machine (SATEC), which was modified to provide constant applied stress, with a variation of no more than 0.7% in the chosen stress. Stresses between 1.6 MPa and 20.5 MPa were applied to the samples producing steady state strain rates between 6.4* 10–9 s–1 to 1.6* 10–2 s–1. The strain during the creep tests was measured with a Schaevitz linear variable differential transformer (LVDT) accurate to±1.3* 10–4 cm, and this information was monitored using a data acquisition system. The test temperatures ranging from 294 K to 398 K were achieved by using tungsten lamps around the specimen holder. This heating device was capable to rise to the selected temperature of the specimen within 20 s. The test temperatures were constant at the level of±0.5 K.The plots of true strain, e, against time, t, which were obtained for specimens with grain sizes of 2.7 μm and 0.6 μm are, respectively illustrated in Figs. 1 and 2. Examination of Fig. 1 corresponding to samples with 2.7 μm has shown that the creep curves exhibit a very short decelerating primary stage followed by a steady state stage; and also exhibit that primary transient strain increases with increasing the applied stress. Unlike our experimental