ct – 3: equilibrium calculations: minimizing of gibbs energy, equilibrium conditions as a set of...
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CT – 3: Equilibrium calculations:
Minimizing of Gibbs energy, equilibrium conditions as a set of equations, global minimization of Gibbs energy, driving force for a phase
Equilibrium conditions
dU = T.dS-p.dV + j j.dnj (see CT-2)Conjugated properties: T,p,j – intensive, S,V,nj – extensive
At constant entropy, volume, and nj , equilibrium is characterized by minimum of the internal energy.
Most proper conditions: p,T,nj
dG = V dp – S dT + j j dnj
(mole fraction: xi = ni/N, N = j nj)
G may have several minima. That with the most negative value of G is „global minimum“ which
corresponds to the „stable equlibrium“ and another ones are „local minima“ and correspond to the „metastable equilibria“
Stable and metastable states
Metastable state
Stable state
Unstable stateUnstable state
Metastable state
Stable state
Equilibrium conditions – cont.
For determination of phases presented in equilibrium: analytical expression of G needed.
Total Gibbs energy:
G = m.Gm (m 0, it is amount of phase )
Amount of components i: Ni = N.xio
Introduce: xi = m. x i - lever rule
Equilibrium condition:
min (G) = min ( m. Gm(T,P, x
i or y (l,)k ))
(xi is definite function of yk
(l, ); m, x i are unknowns)
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• Rule 1: If we know T and Co, then we know: --the composition and types of phases present.
• Example:
wt% Ni20 40 60 80 10001000
1100
1200
1300
1400
1500
1600T(°C)
L (liquid)
(FCC solid solution)
L +
liquidus
solid
us
A(1100,60)B
(1250,3
5)
Cu-Niphase
diagramA(1100, 60): 1 phase:
B(1250, 35): 2 phases: L +
Adapted from Fig. 9.2(a), Callister 6e.(Fig. 9.2(a) is adapted from Phase Diagrams of Binary Nickel Alloys, P. Nash (Ed.), ASM International, Materials Park, OH, 1991).
PHASE DIAGRAMS: composition and types of phases
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• Rule 2: If we know T and Co, then we know: --the composition and amount of each phase.
• Example:
wt% Ni20
1200
1300
T(°C)
L (liquid)
(solid)L +
liquidus
solidus
30 40 50
TAA
DTD
TBB
tie line
L +
433532CoCL C
Cu-Ni system
At TA: Only Liquid (L) CL = Co ( = 35wt% Ni)
At TB: Both and L CL = Cliquidus ( = 32wt% Ni here) C = Csolidus ( = 43wt% Ni here)
At TD: Only Solid () C = Co ( = 35wt% Ni)
Co = 35wt%Ni
Adapted from Fig. 9.2(b), Callister 6e.(Fig. 9.2(b) is adapted from Phase Diagrams of Binary Nickel Alloys, P. Nash (Ed.), ASM International, Materials Park, OH, 1991.)
PHASE DIAGRAMS: composition and amount of phases
Lever rule: mL/m = CoC/CoCL
Equilibrium conditions as a set of equations
Equilibrium condition using chemical potential:
Constraints relating m, xi and Ni used to eliminate
variables m and Ni :
Gi (T,P,xi
) = Gi (T,P,xi
)
(i = 1,…,c, = 1,…p-1, = + 1,…,p)
By the definition:
Gi (T,P,xi
) = i (i = 1,…,c, = 1,…,p)
Nonlinear equations – appropriate iteration algorithm
Unknown: xi and i
(for stoichiometric phases, modifications are necessary)
Gm as function of site fractions yk
(l, )
instead of mole fractions xi
Lagrange-multiplier method
Constraints:
(1) Total amount of each component Ni is kept constant
(2) Sum of site fractions in each sublattice is equal 1
(3) Sum of charge of ionic species in each phase is equal 0
Lagrange-multiplier method-cont.
Each constraint is multiplied by „Lagrange multiplier“ and added to the total Gibbs energy
min (G) = min ( m. Gm(T,P, x
i or y (l,)k ))
to get a sum L.
If all constraints are satisfied, L is equal to G and a minimum of L is equivalent to a minimum of the total Gibbs energy G.
Newton‘s method
To find x for which y=0: (also for searching the minimum of Gm) (df/dx)x=xi . xi = -f(xi), xi+1 = xi + xi There exists cases, where this method diverges
LFS - CT
There exists cases, where Newton‘s method diverges
Starting with x1 - divergesStarting with x3 – solution on the left,
Starting with x4 – solution on the right,
x5, x6 - finally on the left – influence of starting values on the result of minimization
LFS - CT
Newton-Raphson method
It is extension of Newton‘s method to more than one variable (n equations for n unknowns).
All iterative techniques like the Newton-Raphson one need an initial constitution for each phase in order to find the minimum of Gibbs energy surface for the given conditions.
Compounds with fixed compositions
Equilibrium set of phases is given by the tangent „hyperplane“ defined by the Gibbs energies of a set of compounds constrained by the given overall composition and with no compound with a Gibbs energy below this hyperplane („global“ minimum).
Minimization techniques to find global equilibrium
Gibbs energy surface of all solution phases is approximated with a large number of „compounds“ which Gibbs energy has the same value as the solution phase at the composition of the compound (dense grid about 104 (100x100) compounds, for multicomponent system about 106 such compounds)
Search for hyperplane representing equlibrium for the compounds is then carried out.
Minimization techniques to find global equilibrium
When minimum for these „compounds“ has been found, the „compound“ in this equilibrium set must be identified with regard to which solution phase they belong to.
Each „compound“ --- initial constitution of the solution phase --- is used in a Newton-Raphson calculation to find the equilibrium for the solution phases (correct, not wrong)
Limitation of the method to find the global equilibrium
T, p and overall composition must be known
For other conditions as starting point (e.g. activity of components) –-- indirect procedure:
Overall composition calculate first and use it for a new equilibrium calculation.
Conditions for a single equilibrium
The equilibrium conditions as a set of equations contain fewer equation than unknowns – the difference = number of degrees of freedom „f“
Therefore: „f“ extra conditions (equations) must be added to select definitely single equilibrium
„Unknown state variable“ = „constant value“ :
Example:
For binary system i-j: (f=0)
T = 1273, p = 101352, xi = 0.1, i = -40000
Thermocalc: Fe – W – Cr system
set-condition t=1273 x(W)=0.15 x(Cr)=0.35 p=1E5 n=1
Conditions for a single equilibrium – cont.
For each calculation step: which and how many phases are present (Gibbs energy description exist only for phases).
Calculation steps with different sets of phases may be compared
The phases set with lowest Gibbs energy describes the stable equilibrium
Example:
Thermocalc: rej ph * res ph liq bcc fcc sigma Chi R Mu
Example
Different starting points may give different sets of equilibrium phases for the same overall composition.
Check the total Gibbs energy for global minimum
(In new codes checked automatically.)
Output from POLY-3, equilibrium number = 1, Ag-In systemConditions: T=500, X(IN)=2E-1, P=100000, N=1 DEGREES OF FREEDOM 0
Temperature 500.00, Pressure 1.000000E+05 Number of moles of components 1.00000E+00, Mass 1.09260E+02 Total Gibbs energy -3.15128E+04, Enthalpy -1.91077E+02, Volume 0.00000E+00
Overal compositionComponent Moles W-Fraction Activity Potential Ref.state AG 8.0000E-01 7.8982E-01 1.6046E-03 -2.6752E+04 SER
IN 2.0000E-01 2.1018E-01 5.2290E-06 -5.0558E+04 SER FCC_A1#1 Status ENTERED Driving force 0.0000E+00 Number of moles 5.6253E-01, Mass 6.1400E+01 Mass fractions: AG 8.06153E-01 IN 1.93847E-01
HCP_A3#1 Status ENTERED Driving force 0.0000E+00 Number of moles 4.3747E-01, Mass 4.7860E+01 Mass fractions: AG 7.68872E-01 IN 2.31128E-01
Mapping a phase diagram
2 or 3 variables of the conditions are selected as axis variables with lower and upper limit and maximal step.
All additional conditions – kept constant throughout the whole diagram
Start: „initial equilibrium“ for Newton-Raphson calculation (with all phases „entered“)
All results of calculations usually stored – any phase diagram may be displayed at the end of calculations
Mapping a phase diagram – cont.
Example (in Thermocalc):
set-axis-variable 1 x(Ag) 0 1 .025
s-a-v 2 t 300 1200 10
map
(T in K)
„Stepping“
By stepping with small decrements of the temperature (or enthalpy or amount liquid phase-generally one variable) one can determine the new composition of the liquid and then remove the amount of solid phase formed by resetting the overall composition to the new liquid composition before taking the next step
(Scheil solidification scheme: no diffusion in solid phase, high diffusion in liquid phase)
Azeotropic points
Maxima and minima of binary two-phase fields
Setting additional conditions
For binary: x - x = 0
For ternary: xB - xB
= 0
xC - xC
= 0
Driving force-application
Driving force ΔG, GFCC: (Fig.2.5)(difference in G of paralel tangents for phases and
stability tangent)
- theory of nucleation of phases- minimization of G (whether another phases set
exists that is more stable than calculated set of phases)
Conditions for a single equilibrium – cont.
Adding phase to the calculated stable phase set:
Positive „driving force“ of the phase – repeat calculation
Removing phase from the selected set:
Calculation finds negative amount for one of selected phases
Conditions for a single equilibrium – cont.
Phases with miscibility gaps may have more than one driving force at different compositions – test must be performed for each of these compositions
Test by experiment when some phases appear in calculations to be stable but experimentally are found to be not stable
Questions for learning
1.What is a difference between stable and metastable states?
2. What is principle of Lagrange-multiplier method?
3. What is principle of Newton – Raphson method?
4. What conditions must be fulfilled for single equilibrium calculation?
5. What means „mapping“ and „stepping“ in calculations of phase equilibria?