Abstract
The plastic deformation behavior at upper yield point of iron single crystals was studied by the successive stress relaxation method. The specimens used have the same tensile axis [110], but the three specimen groups, of which the upper yield strengths were different from one another, were prepared by controlling carbon content and condition of heat-treatment.
From the results obtained at −61°C, was shown that the true plastic strain rate near the upper yield point can be expressed in terms of the product of two functions: \dotε=f(ε)g(σ), where ε is the plastic strain, and σ the applied tensile stress, the function being the forms of f(ε)∝ε, g(σ)∝σm or g(σ)∝exp(−D⁄σ), where m and D are the constants particular to every specimen group.
On the basis of Johnston-Gilman concept, the contribution of the mobile dislocations to yielding characteristics was examined in terms of the mobility and the density separatedly, and compared in the three specimen groups.