Species Limit Expressions for Order-Disorder Solution Models
To compute the equilibrium speciation of order-disorder models (solution model types 6 and 8)
efficiently, Perple_X requires limits on the physically realizable fractions of the ordered
species. In this context, physically realizable means that the site fractions of every
atom possible on a particular lattice site are greater than or equal to zero. The limits
are entered as a list within a section of the solution model demarked by "begin_limits" and
"end_limits" keywords.
The fully disordered speciation of an order-disorder solution in a c-component composition
space with s-ordered species is uniquely defined by the site populations and stoichiometry
of the c+s endmembers chosen to represent the solution. The fractions of the species for the
disordered composition will be designated p0(1..c+s), while the equilibrium speciation will
be designated p(1..c+s). The bulk composition of each of the s-ordered species can be
described in terms a stoichiometric relationship between c-disordered species (disordered
is a little misleading in this context because it may refer to species in which no
configurational entropy is possible) of the form
ordered_endmember(j) = sum(c(j,i) * disordered_endmember(i), i=1..c), (1)
where ..._endmember(k) denotes the bulk composition of endmember k, and c(j,i) is the
stoichiometric coefficient of the disordered_endmember(i) "in" the ordered_endmember(j).
From (1), for the disordered species (1..c)
p(i) = p0(i) - sum[c(j,i)*[p(j,i) - p0(j,i)], j=c+1..c+s). (2)
Given the known atomic site fractions of every endmember species, the site fraction of
atom k on site l can be expressed
z(k,l) = sum(p(i)*z(k,l,i), i=1..c+s), (3)
where z(k,l,i) is the site fraction of atom k on site l of endmember i. Substituting
(2) into (3) and collecting the stoichiometric factors c(j,i) and z(k,l,i) on a
particular fraction into the coefficient d(k,l,i) yields
z(k,l) = sum(d(k,l,i)*p0(i), i=1..c) + sum(d(k,l,i)*p0(i), i=c+1..c+s)
+ sum(z(k,l,i)*p(i), i=c+1..c+s) (4)
Solving z(k,l) = 0 and z(k,l) = 1 for p(c+1) gives upper and lower, not necessarily
respectively, physically realizable bounds on p(c+1). In Perple_X type 6 and 8 solution
models, the lower bound on the ordered endmember p(c+1) from atom k on site l is written
p(c+1) = f(k,l,c+1)
- d(k,l,1)/z(k,l,c+1)*p0(1) .... - d(k,l,c)/z(k,l,c+1)*p0(c)
- d(k,l,c+1)/z(k,l,c+1) * p0(c+1)
- d(k,l,c+2)/z(k,l,c+1) * p(c+2) - d(k,l,c+2)/z(k,l,c+1) * p0(c+2)
....
- d(k,l,c+s)/z(k,l,c+1) * p(c+s) - d(k,l,c+s)/z(k,l,c+1) * p0(c+s), (5)
where f(k,l,c+1) is a collection of stoichiometric constants, it being assumed that:
1) if the endmember is disordered (i < c + 1), the endmember name represents p0(i).
2) if the expression is for ordered species m, its name occurs only once and represents
p0(m)
3) if the endmember is ordered (i > c) and not the mth ordered species, its name occurs
twice, the first occurence corresponds to p(i) and the second to p0(i).
Because the site fractions are linear in p(i..c+s) the upper and lower abounds differ
by a constant, delta(k,l). Only the expression for the lower bound and the value
for delta(k,l) are specified in Perple_X solution model input. For example for the
Chl(W) (chlorite) solution model with the following endmembers and site occupancies:
M1 M2+M3 M4 T2
________________________________
Mutliplicity 1 4 1 2
________________________________
daph Fe Fe Al Al_Si disordered
f3clin Mg Mg Fe3+ Al_Si disordered
ames Al Mg Al Al_Al disordered
afchl Mg Mg Mg Si_Si disordered
clin Mg Mg Al Al_Si disordered
mnchl Mn Mn Al Al_Si disordered
_______________________________
och1 Mg Fe Fe Si_Si ordered
och2 Fe Mg Mg Si_Si ordered
The site fraction of Mg on lattice site M1 is:
z(Mg,M1) = p(f3clin) + p(afchl) + p(clin) + p(och1)
= p0(f3clin) + p0(afchl) + p0(clin)+ p(och1) - 4/5*p(och2) + 4/5*p0(och2)
and solving Z(Mg,M1) = 1 for p(och2) yields a lower bound of p(och2) as
p(och2) = -5/4 + 5/4*p0(f3clin) + 5/4*p0(afchl) + 5/4*p0(clin) + 5/4*p(och1) + p0(och2)
and in Perple_X input this bound (and the corresponding upper bound) is written
och2 = -5/4 + 5/4 afchl + 5/4 f3clin + 5/4 clin + 5/4 och1 + 1 och2 delta = 5/4
For additional information on the formulation of order-disorder/speciation/compound formation
models refer to chapter 11 of http://www.perplex.ethz.ch/thermo_course/thermo_course.pdf