We investigate a model of dynamic recrystallization in polycrystalline materials. A probability distribution function is introduced to characterize the state of individual grains by grain size and dislocation density. Specifying free energy and dissipation within the polycrystalline aggregate we are able to derive an evolution equation for the probability density function via a thermodynamic extremum principle. Once the distribution function is known macroscopic quantities like average strain and stress can be calculated. For distribution functions which are constant in time, describing a state of dynamic equilibrium, we obtain a partial differential equation in parameter space which we solve using a marching algorithm. Numerical results are presented and their physical interpretation is given.
Mathematical ModelWe investigate the mathematical model based on the work of Hackl and Renner [1] for the phenomenon of dynamic recrystallization in polycrystalline materials. In [1], a probability distribution function f (D, ρ) was introduced, where the state of individual grains is determined by grain size D and dislocation density ρ which we collect into the state variable x = (D, ρ). The distribution function has to satisfy the continuity equation:Moreover the aggregate volume has to be preserved, yielding for spherical grains of diameter D the constraintIn accordance with [1] we assume a specific free energy functional of the formwhere W e is the linear elastic energy, W gb is the grain boundary energy, and W dis is the dislocation energy. The dissipation ∆ is split into the dissipation ∆ p related to plastic deformation, the diffusion-related dissipation ∆ d , the dissipation ∆ D associated with grain coarsening, and the dissipation ∆ ρ associated with a change in dislocation density:Evolution equations for the grain size D and the dislocation density ρ can now be derived employing a thermodynamic extremum principle, see [2], and are given bẏwhere λ is an undetermined constant relating to the Lagrange multiplier of the volume's constraint, γ represents the specific grain boundary energy, δ the width of grain boundary, µ the shear modulus, b the norm of the Burger's vector, a p is a material parameter related to the generation of dislocations, and M ⊥ the diffusion mobility, compare [1]. After inserting (3) and (4) into (1) and (2) and defining the new variable r = 2 √ ρ, we obtainwhere β = µb 2 , η = 4γ, and v = a p δ ε p /4bM ⊥ .