Abstract

The shear behavior of a 6061 aluminum alloy was studied in the semisolid state at large solid fractions. The tests were carried out either at constant temperature after partial solidification (i.e., isothermal shear tests) or during solidification at low cooling rate (i.e., nonisothermal shear tests). In isothermal conditions, results show that (1) the mechanical behavior depends on the volume fraction of the solid phase present in the sample at the temperature of the test, (2) there is a critical solid fraction corresponding to the coalescence of the solid grains beyond which shear stress increases very sharply with increasing solid fraction, and (3) the mushy alloy exhibits viscoplastic behavior with a strain-rate-sensitivity parameter close to about 0.17. In nonisothermal conditions, results show that stress increases continuously with decreasing temperature whatever the strain rate. However, at high strain rate, it was observed that cracks developed when the solid fraction approaches 1, leading to a slower stress increase compared to that observed at low strain rate. Finally, modeling of this behavior is carried out by considering a cohesion parameter of the solid phase, which depends on solid fraction and strain rate.

Highlights

  • SOLIDIFICATION of metallic alloys involves the transformation of the liquid phase into one or more solid phases over a given temperature interval

  • In the case of Al alloys, this transition occurs for solid fractions lower than 0.6.[1,2,4] The second transition separates the domain where the liquid is able to flow between the solid grains from the domain where intergranular flow is no longer possible

  • Isothermal shear tests allow the effects of strain, strain rate, and solid fraction to be investigated in a decoupled manner

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Summary

Introduction

SOLIDIFICATION of metallic alloys involves the transformation of the liquid phase into one or more solid phases over a given temperature interval During this transformation, several transitions are usually defined separating various types of behavior.[1,2,3] The first transition corresponds to the coherency solid fraction, which separates the domain where the solid grains are free to move in the liquid from the domain where they begin to mechanically interact. In the case of Al alloys, this transition occurs for solid fractions lower than 0.6.[1,2,4] The second transition separates the domain where the liquid is able to flow between the solid grains from the domain where intergranular flow is no longer possible At this point, the liquid is present only as films between the solid grains. Several investigations[1,2,4,5,6,7] showed that this transition occurs for solid fractions close to 0.97 in the case of Al alloys

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