动态再结晶
材料科学
再结晶(地质)
热力学
拐点
应变率
奥氏体
热加工
动能
机械
冶金
微观结构
经典力学
数学
古生物学
物理
生物
几何学
作者
Evgueni I. Poliak,John J. Jonas
标识
DOI:10.1016/1359-6454(95)00146-7
摘要
The onset of dynamic recrystallization is treated in terms of a model based on the principles of irreversible thermodynamics. In the analysis, the initiation of dynamic recrystallization is governed by both energetic and kinetic critical conditions. The former requires that the energy stored during a given deformation schedule attain its maximum, while the latter requires the dissipative processes associated with deformation to decelerate to a critical level. The kinetic critical condition leads to a minimum value of ∥−∂θ∂σ∥ (θ is the conventional strain hardening rate) when the critical state is attained and to the appearance of an inflection point in the θ-σ curve. In a range where the strain rate sensitivity is constant, the onset of dynamic recrystallization corresponds to a constant value of Γ = ∂ ln σ∂ϵ. The initiation of dynamic recrystallization has much in common with the beginning of flow localization. These conclusions of the model are verified using experimental data obtained during the high temperature compression of nickel and of a type 305 austenitic stainless steel.
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