The driving force calculation
Posted: Wed Feb 03, 2010 12:04 pm
Hi, Bernd,
According to my understanding, the driving force calculation in MICRESS is done from a parallel tangent construction as,
dG = f(belta)-f(alpha)-mu*(c(belta)-c(alpha)), and mu is defined as diffusion potential
When linking to the real molar Gibbs energy from the CALPHAD-type thermodynamic database, I have two questions as follows (take simple binary as the case),
1) How to get a common mu for both alpha and belta phases to construct a parallel tangent?
2) When one of the phase is described by sublattice model, like (A,B)a(A,B)b, in the database, the site fractions, like y(A)', y(B)', y(A)'' and y(B)'', will be introduced. However, only C(A) or C(B) can be used in the concentration evolution. How do you treat this case in your MICRESS software?
Best wishes!
yours,
sunny
According to my understanding, the driving force calculation in MICRESS is done from a parallel tangent construction as,
dG = f(belta)-f(alpha)-mu*(c(belta)-c(alpha)), and mu is defined as diffusion potential
When linking to the real molar Gibbs energy from the CALPHAD-type thermodynamic database, I have two questions as follows (take simple binary as the case),
1) How to get a common mu for both alpha and belta phases to construct a parallel tangent?
2) When one of the phase is described by sublattice model, like (A,B)a(A,B)b, in the database, the site fractions, like y(A)', y(B)', y(A)'' and y(B)'', will be introduced. However, only C(A) or C(B) can be used in the concentration evolution. How do you treat this case in your MICRESS software?
Best wishes!
yours,
sunny