The Phase Rule
and 1- and 2-Component Systems
(Chapter 6)
last update:09/21/05
Crystallization
behavior of magma from a basaltic lava lake
(Wright and Okamura,
1977)
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Makaopuhi Lava Lake |
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Crystallization Behavior of Melts
1. Cooling melts crystallize from a liquid to a solid over a range of temperatures (and pressures)
2. Several minerals crystallize over this T range, and the number of minerals increases as T decreases
3. The minerals that form do so sequentially, with considerable overlap
4. Minerals that involve solid solution change composition as cooling progresses
5. The melt composition also changes during crystallization
6. The minerals that crystallize (as well as the sequence) depend on T and composition of the melt
7. Pressure can affect the types of minerals that form and the sequence
8. The nature and pressure of the volatiles can also affect the minerals and their sequence
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The Phase Rule
F = C - P + 2
F = # degrees of freedom
The number of intensive parameters that must be specified in order to completely determine the system
P = # of phases
phases are mechanically separable constituents
C = minimum # of components (chemical constituents that must be specified in order to define all phases)
2 = 2 intensive parameters
Usually = temperature and pressure for geologists
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One-component systems
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The SiO2 system. |
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Inclusion of coesite (cs), quartz (qtz)
and chalcedony (cha) in an inclusion within pyrope from Dora Maira Massif
(Italy).
This locality has reached ultrahigh P metamorphic conditions of >30 kb. CL image from a hot-cathode CL system
From Schertl et al. (2004) Eur. J. Mineral. |
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Two-component systems
Binary system with a complete solid solution
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Sample OL-4 - crossed nicols |
Sample OL-4 - Backscattered electron image |

For equilibrium crystallization
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Bulk composition a
= An60
= 60 g An + 40 g Ab XAn = 60/(60+40) = 0.60
1. Must specify 2 independent intensive variables (e.g. T and XAn) in order to completely determine the system = a divariant situation 2. Can vary 2 intensive variables independently without changing P, the number of phases |
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Get new phase joining liquid:
first crystals of plagioclase: = 0.87 (point c)
Must specify only one variable from among: T, XAbLiq, XAbPl, XAnLiq, XAnPl (P = constant) |
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At 1450oC, liquid d
and
plagioclase f coexist at equilibrium
A continuous reaction of the type: liquidA + solidB = liquidC + solidD
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When the composition of solid plagioclase
approaches h, then the solid plagioclase approaches the bulk composition.
The last liquid to crystallize at point g (1340 C) has a composition of An20. |
Equilibrium melting

Fractional
crystallization
(sinking or floating of crystals
as they form)

Another effective manner of fractional crystallization of plagioclase is through compositional zoning such that the An-rich core of a plagioclase is effectively isolated from the liquid (i.e. normal zoning).
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Sample OL-4 - crossed nicols |
Sample OL-4 - Backscattered electron image |
Fractional
or Partial melting
(immediate extraction of melt)

Partial melting will generate a residue plagioclase enriched in An.
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Sample OL-4 - crossed nicols |
Sample OL-4 - Backscattered electron image |
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Fo - Fa (Mg2SiO4 -
Fe2SiO4)
also a solid-solution series
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Binary eutectic systems

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Example: Diopside -
Anorthite |
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(1) a = bulk
composition = An70
(2) Cool to 1455oC (point b) (3) Continue cooling as Xliq varies along the liquidus; (4) Continuous rxn: liqA ® anorthite + liqB |
(5) at 1274oC, P =
3 so F = 2 - 3 + 1 = 0 (invariant)
Discontinuous Reaction: all at a single T |
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Left of the eutectic get a similar situation |
(left) Texture expected to the left of the
eutectic |
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| The last melt to crystallize
in any binary eutectic mixture is the eutectic composition
Equilibrium melting is the opposite of equilibrium crystallization
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For fractional crystallization, the initial crystals will accumulate somewhere and the final melt will be fixed at the eutectic point composition.
For partial melting, the initial melt has the eutectic composition and removed until one the components is removed (An or Di). Then, the remaining solid would be one component and would not melt again until the melting point of the pure phase.
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Binary
Peritectic System
Possible solid phases: Forsterite (Fo) -
Enstatite (En) - Silica (S)
Peritectic reaction:
Mg2SiO4 + SiO2 = 2 MgSiO3
i.e. the composition of En is between Fo and SiO2,
and quartz should never coexist with forsterite!)
Isobaric T-X phase diagram of the system Fo-Silica at 0.1 MPa.
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| For bulk composition f equilibrium crystallization ultimately results in Forsterite + Enstatite |
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i
= "peritectic" point
1557oC have colinear Fo-En-liq
consumes olivine (and liquid) ® resorbed textures
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Fractional crystallization of composition f will generate a layer of Fo, then En and then En + SiO2.
Incongruent Melting of Enstatite (i.e.
Melt of En does not ® melt of same composition
Rather En ® Fo + Liq i at the peritectic
Partial Melting of Fo + En (harzburgite) mantle
En + Fo also ® first liq = i
Remove i and cool
Result = ?
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Pressure Effects
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Solid Solution with a Eutectic
Albite - orthoclase (the alkali feldspar system)
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T-X phase diagram of the system
albite-orthoclase at 0.2 GPa H2O pressure.
The solvus relations of the feldspars are a potential geothermometer
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Effect of PH2O on Ab-Or |
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| At relatively low PH2O, a single feldspar
will crystallize and then undergo further exsolution (a, b) [hypersolvus]
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| At relatively high PH2O, two feldspars will crystallize with possible further exsolution of each phase (c) [subsolvus] | ![]() |