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    An animated introduction to fluidinclusions

    by

    A H RankinSchool of Earth Sciences and Geography

    Kingston University, Surrey KT1 2EE

    http://www.kingston.ac.uk/esg/facilities/fluidinc.ppt

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    The following slides illustrate how primary(P) and secondary (S) inclusions developduring crystal growth and healing ofsecondary fractures

    Aqueous solution

    Crystal

    Some animation has been added

    To see changes hit return

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    Formation of Primary and

    Secondary inclusions

    primary inclusions form during

    primary crystal growth often alonggrowth zones

    secondary inclusions form after primary growth, usually alonghealed micro-fractures

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    P

    S

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    Inclusions formed from trapping of

    homogeneous aqueous fluid will developvapour bubbles on cooling due to differentialthermal contraction of fluid and host mineral.

    The next slide shows groups of two phase(vapour- liquid) primary and secondaryinclusions with distinctly different vapour-

    liquid ratios, indicative of different PTtrapping conditions

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    Contraction vapour bubbles

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    25oC

    0oC

    Vapor

    Liquido

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    The next slides show more complex aqueousinclusions with daughter minerals, liquidcarbon dioxide and liquid hydrocarbons (oil)

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    Multiphase inclusion with daughterand/or captive minerals

    Chalcopyrite halite

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    The halite daughter mineral indicates high salinities (above26 wt.%) which may be estimated from the solutiontemperature of halite.

    The chalcopyrite crystal here is either a captive or truedaughter phase. But such opaque minerals are reluctant todissolve even if they are true daughters

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    CO 2-rich aqueous inclusion

    CO 2 vapour CO 2 Liquid

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    Liquid CO 2 will only be seen in the inclusion below the critical point of CO 2 (31 oC).

    On cooling the CO 2 will react with water toform clathrates (ice like compounds).

    On more rapid cooling solid CO 2 will form. If pure, melting will occur at the triple point of

    CO 2 (-56.6o

    C). If other volatiles, e.g. nitrogenor methane, are present the meltingtemperature will be lowered

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    Oil-water inclusion

    Vapour Oil

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    Liquid petroleum may be identified as an immiscible phasewithin an inclusion, by its brownish colour or UVfluorescence (as shown in the next slide)

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    The following slides show the homogenisation

    of liquid and vapour in a two phase aqueousinclusion during laboratory heating. Thetemperature at which this occurs is the

    Homogenisation temperature (Th) The bubblereturns on cooling.Heating

    Cooling

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

    Temperature of Homogenisation Th

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    -100 oC

    0oC

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    350 oC

    25oC

    0oC

    -100 oCFreezing after Supercooling

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oC

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    350 oC

    25oC

    0oC

    -100 oCLast ice melting temperature Tm(ice)

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    The next slides illustrate the use of heating and freezing datafor simple two phase aqueous inclusions.

    Heating and freezing data (Th, Tfm, Tmice) are interpreted in

    terms of the simple H 2O and NaCl-H 2O systems

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    Principle of fluid inclusion geothermometry

    PVT diagram for pure water 1.0

    0.5

    0

    50 150 350

    Isochore(g/cc)

    Critical point

    Liquid

    Vapour

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    Consider an inclusion trapped at a giventemperature and pressure (Tt, Pt)

    1.0

    0.5

    0

    50 150 350 Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    Beyond this point the inclusion cools alongthe L=V curve and a vapour bubble nucleates

    1.0

    0.5

    0

    50 150 350 Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    Continued cooling results in further shrinkageof liquid and growth of the vapour bubble

    1.0

    0.5

    0

    50 150 350 Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    On heating along the V/L curve, the liquidexpands and the bubble shrinks

    1.0

    0.5

    0

    50 150 350 Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    Until the bubble disappears at the

    homogenisation temperature (Th) 1.0

    0.5

    0

    50 150 350 Th Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    The point Th uniquely defines the isochorealong which the inclusions originally cooled1.0

    0.5

    0

    50 150 350 Th Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    With continued heating the inclusion followsthe original isochore

    1.0

    0.5

    0

    50 150 350 Th Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    The difference between Th and Tt is known asthe Pressure Correction

    1.0

    0.5

    0

    50 150 350 Th Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

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    The bubble reappears on cooling and Th can be re-determined

    1.0

    0.5

    0

    50 150 350 Th Tt

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour

    Phase diagram for NaCl-H2O showing stability

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ V

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    3020100

    Phase diagram for NaCl H2O showing stabilityfields for halite, hydrohalite, liquid and vapour

    An inclusion with 10 wt.% solution cooled below

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ V

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    3020100

    An inclusion with 10 wt.% solution cooled below0oC does not form ice because of metastability

    Rapid cooling below the eutectic temperature (Te)

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ V

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    3020100

    ap d coo g be ow t e eutect c te pe atu e ( e)is usually needed before the inclusion freezes

    On heating first melting (Tfm) occurs at -20.8

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ VTfm

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    3020100

    g g ( )(Te), evident by unlocking of the vapour bubble

    Continued heating results in the melting of the last

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ VTfm

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    Tm (ice)

    3020100

    g gice crystal (Tm_ice) at -6 oC

    Continued heating results in the melting of the last

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    0.1 oC

    -20.8 oC

    Ice + NaCl.2H 2O + V

    Ice + L+ V

    L + V NaCl+L+V

    NaCl.2H 2O+L+ VTfm

    Weight % NaCl

    T e m p e r a t u r e

    o C

    -50

    25

    -25

    0

    Tm (ice)

    3020100

    g gice crystal (Tm_ice) at -6 oC

    Principle of fl id incl sion geothermometr

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    Principle of fluid inclusion geothermometry

    based on PVT diagram for pure water 1.0

    0.5

    0

    PtIsochore(g/cc)

    Critical point

    Liquid

    Vapour