7 FASES TERNARIAS

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    C = 3: Ternary Systems:Example 1: Ternary Eutectic

    Di - An - Fo

    T

    M

    Anorthite

    Forsterite

    Diopside

    Note three binary eutectics

    No solid solution

    Ternary eutectic = M

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    T - X Projection of Di - An - Fo

    Figure 7-2. Isobaric

    diagram illustrating

    the liquidus

    temperatures in the

    Di-An-Fo system at

    atmospheric pressure(0.1 MPa). After

    Bowen (1915), A. J.

    Sci., and Morse

    (1994), Basalts and

    Phase Diagrams.

    Krieger Publishers.

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    Crystallization Relationships

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    An + Liq

    Liquid

    Di + Liq

    Di + An

    a

    An

    Pure Fo formsJust as in binary

    f = ?

    F = ?

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    f = 2 (Fo + Liq)

    F = 3 - 2 + 1 = 2

    If on liquidus, need to specify

    only 2 intensive variables

    to determine the system

    T and or

    and

    X of pure Fo is fixed

    XAnliq

    XAnliq

    XFoliq

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    Lever principle relative proportions of liquid & Fo

    At 1500oC

    Liqx + Fo = bulka

    x/Fo = a-Fo/x-a

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    New continuous reaction as liquid follows cotectic:

    LiqA LiqB + Fo + Di

    Bulk solid extract Di/Fo in bulk solid extract using lever principle

    1274

    1392

    Diopside

    M

    b

    c

    Fo + Liq

    1387

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    At 1300oC liquid = X

    Imagine triangular plane X - Di - Fo balanced on bulk a

    Liq/total solids = a-m/Liq-a

    total Di/Fo = m-Fo/Di-m

    a

    Di

    L iq x

    Fom

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    Partial Melting(remove melt):

    i i

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    Ternary Peritectic Systems:(at 0.1 MPa)

    Figure 7-4. Isobaric

    diagram illustrating

    the cotectic and

    peritectic curves in

    the system forsterite-

    anorthite-silica at 0.1

    MPa. After Anderson

    (1915) A. J. Sci., and

    Irvine (1975) CIW

    Yearb. 74.

    3 binary systems:

    Fo-An eutecticAn-SiO2 eutectic

    Fo-SiO2 peritectic

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    1890Fo En

    a

    b

    y

    x

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    Works the same way as the Fo - En - SiO2 binary

    ik

    Fo En

    1557

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    Fo En

    e b

    f

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    Diopside-Albite-Anorthite

    Di - An Eutectic

    Di - Ab Eutectic

    Ab - An solid solution

    Figure 7-5. Isobaric

    diagram illustrating theliquidus temperatures

    in the system diopside-

    anorthite-albite at

    atmospheric pressure

    (0.1 MPa). After Morse

    (1994), Basalts and

    Phase Diagrams.Krieger Publushers

    Figure 7-5 Isobaric

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    Isobaric

    polythermalprojection

    Figure 7-5. Isobaric

    diagram illustrating the

    liquidus temperatures in

    the system diopside-

    anorthite-albite at

    atmospheric pressure

    (0.1 MPa). After Morse

    (1994), Basalts andPhase Diagrams. Krieger

    Publishers.

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    Note:

    Binary character is usually maintainedwhen a new component is added

    Eutectic behavior remains eutectic

    Peritectic behavior remains peritectic

    Solid solutions remain so as well

    Obli

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    Oblique

    ViewIsothermal

    Section

    Figure 7-8. Oblique view illustrating an isothermal section through the diopside-albite-anorthite

    system. Figure 7-9. Isothermal section at 1250oC (and 0.1 MPa) in the system Di-An-Ab. Both fromMorse (1994), Basalts and Phase Diagrams. Krieger Publishers.

    T F ld

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    Ternary Feldspars

    1118

    Ab 20 40 60 80 An

    1100

    1200

    1300

    1400

    1500

    1557

    T Co

    PlagioclaseLiquid

    Liquid

    plus

    Weight % An

    Plagioclase

    OrAb

    Ab-rich feldspar

    + liquid

    liquid

    single feldspar

    two feldspars

    1200

    1000

    800TemperatureoC

    Wt.%

    a

    cb

    de

    f

    g h

    i

    jk

    Figure 7-10. After Carmichael et al.(1974), Igneous Petrology. McGraw Hill.

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    Ternary Feldspars

    Trace of solvus

    at three

    temperature

    intervals

    Triangle shows coexisting

    feldspars and liquid at

    900oC

    Figure 7-11. Winter (2001) An

    Introduction to Igneous and

    Metamorphic Petrology. PrenticeHall.

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    4 - Component Diagrams

    An

    Figure 7-12. The system

    diopside-anorthite-albite-forsterite. After

    Yoder and Tilley (1962).

    J. Petrol.

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    > 4 Components

    Figure 7-13. Pressure-temperature

    phase diagram for the melting of a

    Snake River (Idaho, USA) tholeiitic

    basalt under anhydrous conditions.

    After Thompson (1972). Carnegie

    Inst. Wash Yb. 71

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    olivine Calcic plagioclase

    Mg pyroxene

    Mg-Ca pyroxene

    amphibole

    biotite

    (Spinel)

    potash feldsparmuscovite

    quartz

    alkalic plagioclase

    Calci-alkalic plagioclase

    alkali-calcic plagioclase

    Bowens Reaction Series

    Discontinuous

    Series

    ContinuousSeries

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    The Effect of Pressure

    Liquid

    Temperature

    Solid

    P1

    P2

    T1 T2

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    Eutectic system

    Figure 7-16. Effect of lithostatic pressure on the liquidus and eutectic composition in the diopside-anorthite system. 1 GPa data from Presnall et al. (1978). Contr. Min. Pet., 66, 203-220.

    Th Eff t f W t M lti

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    The Effect of Water on MeltingDry melting:solid liquid

    Add water- water enters the meltReaction becomes:

    solid + water = liq(aq)

    Figure 7-19. The effect of H2O

    saturation on the melting of albite,

    from the experiments by Burnham

    and Davis (1974). A J Sci 274, 902-

    940. The dry melting curve is

    from Boyd and England (1963).JGR 68, 311-323.

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    Figure 7-20. Experimentally determined melting intervals of gabbro under H2O-free (dry), andH2O-saturated conditions. After Lambert and Wyllie (1972). J. Geol., 80, 693-708.

    Dry and water saturated solidi for some common rock types

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    Dry and water-saturated solidi for some common rock types

    The more mafic the rock

    the higher the melting

    point

    All solidi are greatly

    lowered by water

    Figure 7-21. H2O-saturated (solid)

    and H2O-free (dashed) solidi

    (beginning of melting) for

    granodiorite (Robertson and Wyllie,

    1971), gabbro (Lambert and Wyllie,

    1972) and peridotite (H2O-saturated:

    Kushiro et al., 1968; dry: Ito andKennedy, 1967).

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    We know the behavior of water-free and water-saturated

    melting by experiments, which are easy to control by

    performing them in dry and wet sealed vessles

    What about real rocks?

    Some may be dry, some saturated, but most are morelikely to be in between these extremes

    a fixed water content < saturation levels

    a fixed water activity

    Th Albit W t

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    The Albite-Water

    System

    Red curves = melting for

    a fixed mol % water in

    the melt (Xw)

    Blue curves tell the water

    content of a water-

    saturated melt

    m

    Figure 7-22. From Burnham and Davis(1974). A J Sci., 274, 902-940.

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    Raise a melt with a ratio

    of albite:water = 1:1

    (Xwater= 0.5)

    from point a at 925

    o

    C and1 GPa pressure, toward the

    Earths surface under

    isothermal conditions.

    melt

    Figure 7-22. From Burnham and Davis(1974). A J Sci., 274, 902-940.

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    Conclusions:

    A rising magma witha fixed % water will

    progressively melt

    At shallower levels it

    will become saturated,

    and expel water into

    its surroundings

    Figure 7-22. From Burnham and Davis(1974). A J Sci., 274, 902-940.

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    Another example: isobaric

    heating of albite with

    10 mol % water at 0.6 GPa.

    Figure 7-22. From Burnham and Davis(1974). A J Sci., 274, 902-940.

    15% 20% 50% 100%

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    Conclusion:

    Although the addition of

    water can drastically reduce

    the melting point of rocks,the amount of melt produced

    at the lower temperature may

    be quite limited, depending

    on the amount of wateravailable

    Figure 7-22. From Burnham and Davis(1974). A J Sci., 274, 902-940.

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    Melting of Albite with a

    fixed activity of H2O

    Fluid may be a CO2-H2O

    mixture with Pf= PTotal

    Figure 7-23. From Burnham and Davis(1974). A J Sci., 274, 902-940.

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    Melting of Albite with a

    fixed activity of H2O

    Fluid may be a CO2-H2O

    mixture with Pf= PTotal

    Figure 7-26. From Millhollen et al. (1974). J. Geol., 82, 575-587.

    Th l bilit f t i lt d d th t t f

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    The solubility of water in a melt depends on the structure of

    the melt (which reflects the structure of the mineralogical

    equivalent)

    Figure 7-25. The effect of H2O on the

    diopside-anorthite liquidus. Dry and 1

    atm from Figure 7-16, PH2O = Ptotal curve

    for 1 GPa from Yoder (1965). CIW Yb 64.

    Effect of Pressure Water and CO on the position

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    Ne

    Ab

    Oversaturated(quartz-bearing)tholeiitic basalts

    Highly undesaturated(nepheline-bearing)

    alkali olivinebasalts

    3GPa2GPa

    1GPa

    1atm

    Volatile-free

    Ne

    Ab

    Oversaturated(quartz-bearing)tholeiitic basalts

    Highly undesaturated(nepheline-bearing)

    alkali olivinebasalts

    CO2

    H2Odry

    P = 2 GPa

    Effect of Pressure, Water, and CO2 on the position

    of the eutectic in the basalt system

    Increased pressure moves the

    ternary eutectic (first melt) fromsilica-saturated to highly undersat.

    alkaline basalts

    Water moves the (2 GPa) eutectic

    toward higher silica, while CO2

    moves it to more alkaline types