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MTDATA Demonstration : Oxide Systems
Contents
Introduction
A knowledge of phase equilibria in multicomponent
oxide systems is important in a great many fields. These include
pyro-metallurgy, energy conversion, the prevention of corrosion,
pollution control and the formulation, manufacture and use of cements
and refractories.
This demonstration shows how MTDATA can be used to
predict phase equilibria in complex oxide systems using critically
assessed thermodynamic data. Compositions, temperatures, pressures and
other conditions have been chosen to relate as closely as possible to
industrial practice. Of course these can be varied easily from within
MTDATA to suit any particular application.
The data used were developed as part of an ongoing
project sponsored through MIRO. Its aim is to cover the CaO-MgO-Fe-O-Al2O3-SiO2
system and then add other important sub-systems such as those involving
as copper, zinc and sulphur.
The CaO-SiO2 system
Data for multicomponent oxide systems are built up
from those for much simpler sub-systems. The CaO-SiO2
system is a particularly important building block because lime and
silica are almost universal components of pyrometallurgical slags.
Predicted invariant temperatures are superimposed
on the calculated CaO-SiO2 phase diagram along
with accepted experimental values. The REPLOT command is used to do
this.
Note that in defining the system to be studied
charge (O/-2) is included as a component. This enables charged species
to be retrieved from the database.
WHICH MODULE ? BINARY BINARY OPTION ? DEFINE SYSTEM 'CaO,SiO2,O/-2' SOURCE OXIDE ! SEARCHING FOR SYSTEM CaO,SiO2,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. BINARY OPTION ? CLASSIFY MISCIBILITY(LIQUID) 1 ! BINARY OPTION ? STEP TEMPERATURE 1200 3200 20 ! COMPUTE ! BINARY OPTION ? REPLOT EXPERIMENTAL_FILE 'CS.EXP' GO
The Al2O3-SiO2
system
It is difficult to study the Al2O3-SiO2
system experimentally because of its high liquidus temperatures and the
viscosity of the melts involved. The variation in the experimental data
points superimposed on the silica rich end of the calculated phase
diagram reflects this fact. Fortunately good data relating to the
extent of the mullite phase field are available. These have been taken
into account in modelling mullite crystalline solutions and their
relationships with other phases.
It is interesting to note that by classifying
certain phases absent (ie not to be considered in calculations) MTDATA
can be used to investigate metastable phase equilibria. The region of
metastable liquid immiscibility shown just below the silica rich
liquidus was mapped in this way. Experimental evidence for metastable
immiscibility in silica rich liquids has been reported in the
scientific literature.
BINARY OPTION ? DEFINE SYSTEM 'Al2O3,SiO2,O/-2' SOURCE OXIDE OUTPUT 'AS.MPI' ! SEARCHING FOR SYSTEM Al2O3,SiO2,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. BINARY OPTION ? CLASSIFY MISCIBILITY(LIQUID) 1 ! BINARY OPTION ? STEP TEMPERATURE 1600 2400 20 ! COMPUTE ! BINARY OPTION ? REPLOT EXPERIMENTAL_FILE 'AS.EXP' GO
The CaO-Al2O3-SiO2
system
Data for ternary oxide systems such as CaO-Al2O3-SiO2
are based upon those for the component binaries (CaO-SiO2,
CaO-Al2O3, Al2O3-SiO2)
with ternary parameters added where necessary to reproduce experimental
observations. Phase equilibria are usually calculated at a single
temperature and plotted on a triangular grid. (Note that the SET W=1
command is used to request a diagram plotted in weight fractions rather
than mole fractions).
The chosen temperature of 1800 K (1527 C) is just
below the melting points of both pseudowollastonite and anorthite.
Consequently rather small phase fields are associated with each of
these compounds. At this temperature melts exhibit silica contents
ranging between zero and about 95 weight percent silica. Silica rich
and silica poor liquids are separated by a region of coexistence with
the compound melilite (gehlenite).
The compound hatrurite (tricalcium silicate) is a
major component of Portland Cement. It is stable in equilibrium with
the liquid phase either alone or in conjunction with alpha dicalcium
silicate or lime. (To allow lime to form crystalline solutions with
other compounds of similar structure, eg wustite, it is given the
generic phase name halite in MTDATA databases).
BINARY OPTION ? RETURN WHICH MODULE ? TERNARY TERNARY OPTION ? DEFINE SYSTEM 'CaO,SiO2,Al2O3,O/-2' SOURCE OXIDE ! SEARCHING FOR SYSTEM CaO,SiO2,Al2O3,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. TERNARY OPTION ? CLASSIFY MISCIBILITY(LIQUID) 1 ! TERNARY OPTION ? SET TEMPERATURE 1800 W 1 ! COMPUTE !
The Fe-O-SiO2 system
When present in slags iron always occurs in both
ferrous and ferric forms. This means that FeO must always be considered
together with Fe2O3 and
Fe in calculating phase equilibria for iron containing systems.
At 1475 K (1202 C) in the FeO-SiO2-Fe2O3
system a small region of single phase liquid exists. Compositions along
the left hand boundary of this region, are those for which either pure
iron or the compound fayalite will separate out from the slag (liquid)
phase on reduction. The lines extending outside the ternary triangle to
the left correspond to equilibria involving pure iron (the FCC_A1
phase). Iron itself cannot be represented within the FeO-SiO2-Fe2O3
composition triangle.
Towards the right of the diagram, under more
oxidising conditions, the spinel phase (magnetite) and haematite become
stable. (To allow for possible crystalline solution with Al2O3,
haematite is given the generic phase name corundum in MTDATA databases).
TERNARY OPTION ? DEFINE SYSTEM 'FeO,SiO2,Fe2O3,O/-2' SOURCE OXIDE ! SEARCHING FOR SYSTEM FeO,SiO2,Fe2O3,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. TERNARY OPTION ? SET TEMPERATURE 1475 W 1 ! COMPUTE !
The Fe-O-Al2O3
system in air
Since mixtures of "iron oxide" and alumina do not
constitute a true binary system (due to the presence of both ferrous
and ferric iron) the BINARY module of MTDATA cannot be used to
calculate a phase diagram for this system. Instead a facility within
the APPLICATION module is used. This enables temperature sections
(isopleths) to be plotted along a chosen line through any
multicomponent system.
Phase equilibria can be calculated for any
selected oxygen pressure. To do this gas phase data for O2
are introduced and an appropriate overall pressure imposed. An oxygen
pressure of about 0.21 atmospheres corresponds to that in air.
In the Fe-O-Al2O3
system under such conditions the compound Al2O3.Fe2O3
is stable over a limited temperature range above about 1590 K. At lower
temperatures corundum crystalline solutions rich in Al2O3
coexist with those rich in Fe2O3
(haematite). At higher temperatures, until the liquid phase forms, the
spinel phase becomes the main carrier of iron. The next two examples
illustrate the care taken in modelling the structure and properties of
this complex phase.
TERNARY OPTION ? RETURN WHICH MODULE ? APPLICATION APPLICATION OPTION ? DEFINE SYSTEM 'FeO,Fe2O3,Al2O3,O/-2' SOURCE OXIDE % ? OUTPUT 'WFA' ! SEARCHING FOR SYSTEM FeO,Fe2O3,Al2O3,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. APPLICATION OPTION ? CLASSIFY MISCIBILITY(CORUNDUM) 1 MISC(SPINEL) 1 ! APPLICATION OPTION ? SET P 0.21*101325.0 ! APPLICATION OPTION ? 'ISOPLETH.MAC Isopleth - the calculation of pseudo binary sections through multicomponent systems It is now necessary to define certain parameters for the calculations. Enter composition tolerance (typically 0.0001) ? : 0.0001 Enter number of temperature steps (perhaps 30) ? : 50 APPLICATION OPTION ? SET W 1 "Fe2O3" 0.0 1.0 0.0 "Al2O3" 0.0 0.0 1.0 ! APPLICATION OPTION ? RANGE "Fe2O3" "Al2O3" 50 ! APPLICATION OPTION ? RANGE TEMPERATURE 1100 2500 0.1 ! COMPUTE !
In the above commands Fe2O3
and Al2O3 are used as
labels for the corresponding compositions.
Cation distribution in Fe-O-Al2O3
spinels
Two types of cation site exist within the spinel
structure; tetrahedrally co-ordinated and octahedrally co-ordinated
sites. For each site of the first type there are two of the second. In
a "normal" spinel divalent ions (A) occupy all the tetrahedral sites
and trivalent ions (B) all the octahedral sites so giving an overall
formula AB2O4.
Alternatively the tetrahedral sites may be occupied by trivalent ions
and half the octahedral sites by divalent ions. The spinel is then said
to be "inverse".
The calculated cation distribution along the join
between Fe3O4 (magnetite)
and FeAl2O4 (hercynite)
at 1273 K shows hercynite to be approximately normal with Al3+
ions occupying octahedral sites and Fe2+ ions
tetrahedral sites. In contrast magnetite exhibits a mixed structure
with significant populations of both ferric and ferrous ions on the
tetrahedral sites.
These results are in good agreement with the
somewhat scattered measurements of cation distributions shown
superimposed upon the calculated curves.
APPLICATION OPTION ? RETURN WHICH MODULE ? MULTIPHASE MULTIPHASE OPTION ? DEFINE DATA_INPUT_FILE 'WFA' ! MULTIPHASE OPTION ? CLASSIFY ABSENT PHASE(*) NORMAL PHASE(SPINEL) ! MULTIPHASE OPTION ? SET TEMPERATURE 1273 ! MULTIPHASE OPTION ? SET 'Fe3O4' 1.0 1.0 0.0 'FeAl2O4' 1.0 0.0 1.0 ! MULTIPHASE OPTION ? STEP 'Fe3O4' 'FeAl2O4' 51 ! MULTIPHASE OPTION ? COMPUTE PRINT GRAPHICS ! 51 MOLE STEPS JOINING Fe3O4 TO FeAl2O4 MULTIPHASE OPTION ? ORDINATE N_(AMOUNT) SUBSTANCE(SPINEL) LIMITS 0.0 2.0 ! MULTIPHASE OPTION ? PLOT GO
Miscibility gap in the spinel phase
Below about 1130 K spinels rich in alumina
(hercynite like) and spinels poor in alumina (magnetite like) separate
to form two immiscible phases. MTDATA can be used to plot composition
limits for this immiscibility.
The calculated solvus lies within the error bounds
of all the superimposed experimental data points. Note the slight bulge
in the calculated phase boundary below about 800 K close to the
composition of magnetite (Fe3O4).
This is a manifestation of magnetic contributions to the Gibbs energy
of iron rich spinels becoming significant.
MULTIPHASE OPTION ? RETURN WHICH MODULE ? APPLICATION APPLICATION OPTION ? DEFINE DATA_INPUT_FILE 'WFA' ! APPLICATION OPTION ? CLASSIFY ABSENT PHASE(*) MISCIBILITY(SPINEL) 1 ! APPLICATION OPTION ? 'ISOPLETH.MAC Isopleth - the calculation of pseudo binary sections through multicomponent systems It is now necessary to define certain parameters for the calculations. Enter composition tolerance (typically 0.0001) ? : 0.0001 Enter number of temperature steps (perhaps 30) ? : 50 APPLICATION OPTION ? SET "Fe3O4" 0.5 0.5 0.0 "FeAl2O4" 0.5 0.0 0.5 ! APPLICATION OPTION ? RANGE "FeAl2O4" "Fe2O3" 50 ! APPLICATION OPTION ? RANGE TEMPERATURE 700 1300 0.1 ! COMPUTE !
The CaO-Fe-O-Al2O3
system at 1418 K
Under oxidising conditions (in air for example)
and at temperatures low enough to exclude the spinel and liquid phases,
most of the iron in the CaO-Fe-O-Al2O3
system occurs in the ferric form. As a result the phase equilibria
appropriate to such conditions can be represented, to a good
approximation, on the CaO-Fe2O3-Al2O3
ternary grid.
The ternary section calculated at 1418 K is
dominated by the relationships between the calcium ferrites (C2F and
CF) each of which dissolves alumina to some extent and a series of
calcium aluminates (C3A, C12A7, CA, CA2 and CA6) all of which dissolve
some ferric oxide. A ternary compound with the approximate formula CAF2
is also formed. (In these formulae C is used to represent CaO, A to
represent Al2O3 and F to
represent Fe2O3). A
miscibility gap in the corundum phase (Al2O3
in equilibrium with haematite) is apparent along the Al2O3-Fe2O3
binary edge.
The calculated phase fields at this temperature
are in excellent agreement with those observed experimentally. The
experimental equilibria are identified by a series of symbols
superimposed upon the calculated diagram.
APPLICATION OPTION ? RETURN WHICH MODULE ? TERNARY TERNARY OPTION ? DEFINE SYSTEM 'CaO,Fe2O3,Al2O3,O/-2' SOURCE OXIDE ! SEARCHING FOR SYSTEM CaO,Fe2O3,Al2O3,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. TERNARY OPTION ? CLASSIFY MISCIBILITY(CORUNDUM) 1 ! TERNARY OPTION ? SET TEMPERATURE 1418 W 1 ! COMPUTE !
Section across the CaO-Fe-O-Al2O3
system between C4AF and C5A3
In studying the way phase equilibria in a
multicomponent system change with temperature it is useful to be able
to plot pseudo-binary sections between compositions of practical
interest. An example of such a calculation is the following section
across the CaO-Fe-O-Al2O3
system between C4AF and C5A3 at 0.21 atmospheres O2
pressure.
The liquidus takes the form of a eutectic valley
with CA as the primary phase close to C5A3 and C2F as the primary phase
close to C4AF. Both CA and C2F exist as a series of crystalline
solutions. The composition at the bottom of the valley (48 weight %
CaO, 10 weight % Fe2O3
and 42 weight % Al2O3)
agrees closely with that determined experimentally.
Since this is not a true binary diagram but a
section through a multicomponent system, more than two phases may be
found to coexist in some regions. The crystalline solutions CA, C12A7
and C2F at low temperatures are one example. Furthermore tie-lines in
two phase fields do not necessarily lie in the plane of the diagram as
would be the case for a true binary system.
TERNARY OPTION ? RETURN WHICH MODULE ? APPLICATION APPLICATION OPTION ? DEFINE SYSTEM 'CaO,Fe2O3,Al2O3,O2,O/-2' SOURCE OXIDE % ? OUTPUT 'CWFA.MPI' ! SEARCHING FOR SYSTEM CaO,Fe2O3,Al2O3,O2,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. APPLICATION OPTION ? 'ISOPLETH.MAC Isopleth - the calculation of pseudo binary sections through multicomponent systems It is now necessary to define certain parameters for the calculations. Enter composition tolerance (typically 0.0001) ? : 0.0001 Enter number of temperature steps (perhaps 30) ? : 50 APPLICATION OPTION ? SET "C4AF" 0.46113 0.32827 0.20960 0.001 ! APPLICATION OPTION ? SET "C5A3" 0.47773 0.0001 0.52117 0.001 ! APPLICATION OPTION ? SET W 1 ! RANGE "C4AF" "C5A3" 50 ! APPLICATION OPTION ? RANGE TEMPERATURE 1400 1750 0.1 ! COMPUTE !
FeO activities in the Fe-O-SiO2-Al2O3
system
Phase equilibrium calculations in a multicomponent
system can be analyzed in a great many ways. MTDATA, for example, can
be used to study a variety of thermodynamic functions as well as for
examining the stability of phase combinations as already shown. Such
functions include the activity of individual components relative to a
chosen reference state.
In the following diagram FeO activities at 1673 K
are plotted along a line through the Fe-O-SiO2-Al2O3
system joining a 92:8 mixture of SiO2 and Al2O3
with pure iron oxide in contact with iron. At high iron oxide
concentrations the only stable oxide phase is the liquid. For such
compositions the variation in FeO activity with the mole fraction of
FeO is markedly non-linear and a pronounced hump is evident in the
calculated activity curve. This is in good agreement with the
superimposed experimental data points.
At higher SiO2 and Al2O3
concentrations, of less importance practically, first tridymite, then
tridymite and mullite are formed along with the liquid phase. Agreement
between calculation and experiment is not as good for these
compositions. Note however that some variation is apparent in the
experimental data points.
APPLICATION OPTION ? RETURN MULTIPHASE MULTIPHASE OPTION ? DEFINE SYSTEM 'FeO,SiO2,Al2O3,Fe,O/-2' SOU OXIDE ! SEARCHING FOR SYSTEM FeO,SiO2,Al2O3,Fe,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. MULTIPHASE OPTION ? CLASSIFY REFERENCE(2) 1 ! SET TEMPERATURE 1673 ! MULTIPHASE OPTION ? SET 'S92A8' 0.0 0.92 0.08 0.001 'FeO' 1.0 0.0 0.0 0.001 ! MULTIPHASE OPTION ? STEP 'S92A8' 'FeO' 51 ! COMPUTE PRINT GRAPHICS ! 51 MOLE STEPS JOINING S92A8 TO FeO MULTIPHASE OPTION ? ORDINATE COMPONENT_ACTIVITY COMPONENT(FeO) ! PLOT GO
The iron cordierite primary phase field
Liquidus contours and primary phase maps are a
convenient way of picturing high temperature phase equilibria in
systems with three or more components. A relatively new feature of
MTDATA allows these sorts of diagram to be drawn for any composition
triangle within a multicomponent system. Liquidus temperatures are
calculated and primary phases identified at all points on a grid
spanning three chosen compositions. Contours are then constructed based
upon these results.
In the Fe-O-SiO2-Al2O3
system in contact with iron, the compound iron cordierite (Fe2Al4Si5O18)
appears as the primary crystalline phase over a rather limited range of
composition. This is sandwiched between two much more extensive primary
phase fields corresponding to spinel (hercynite) crystalline solutions
and cristobalite. The ends of the iron cordierite field, less then 1
weight % SiO2 wide, are capped by fields
corresponding to fayalite and mullite.
The liquidus contours superimposed on the primary
phase map suggest that iron cordierite occurs as a primary phase over a
temperature range of less than 150 K.
MULTIPHASE OPTION ? RETURN WHICH MODULE ? APPLICATION APPLICATION OPTION ? DEFINE SYSTEM 'FeO,SiO2,Al2O3,Fe,O/-2' SOURCE OXIDE ! SEARCHING FOR SYSTEM FeO,SiO2,Al2O3,Fe,O/-2 oxide - NPL oxide database. Vers. 2.0. 1997. APPLICATION OPTION ? SET P 0.21*101325.0 W 1 ! APPLICATION OPTION ? SET 'W5S4A1' 0.5 0.4 0.1 0.0001 ! APPLICATION OPTION ? SET 'W3S6A1' 0.3 0.6 0.1 0.0001 ! APPLICATION OPTION ? SET 'W3S4A3' 0.3 0.4 0.3 0.0001 ! APPLICATION OPTION ? RANGE T 2500 1300 0.1 ! APPLICATION OPTION ? 'LIQUIDUS Liquidus - liquidus contours and primary phase fields for ternary slices through multicomponent systems It is now necessary to define certain parameters for the calculations. Enter name of composition to be plotted lower left ? : 'W5S4A1' Enter name of composition to be plotted at the top ? : 'W3S6A1' Enter name of composition to be plotted lower right ? : 'W3S4A3' Enter number of steps between each composition ? : 50 Enter contour interval required ? : 50 APPLICATION OPTION ? COMPUTE !
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