ch13 phase diagrams

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    TRANSITIONS BETWEEN PHASES

    See the phase diagram for water, Figure 13.37.

    Lines connect all conditions of T and P whereEQUILIBRIUM exists between the phases on either side

    of the line.

    (At equilibrium particles move from liquid to gas as fast

    as they move from gas to liquid, for example.)

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    Copyright (c) 1999 by Harcourt Brace & Company

    All rights reserved

    Phase Diagram for Water

    Animation of

    solid phase.

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    Copyright (c) 1999 by Harcourt Brace & Company

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    Phase Diagram for Water

    Animation of

    equilibriumbetweensolid andliquid

    phases.

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    Copyright (c) 1999 by Harcourt Brace & Company

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    Phase Diagram for Water

    Animation of

    liquid phase.

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    Copyright (c) 1999 by Harcourt Brace & Company

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    Phase Diagram for Water

    Animation of

    equilibriumbetweenliquid andgas phases.

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    Copyright (c) 1999 by Harcourt Brace & Company

    All rights reserved

    Phase Diagram for Water

    Animation of

    gas phase.

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    Copyright (c) 1999 by Harcourt Brace & Company

    All rights reserved

    Phase Diagram for Water

    Animation of

    equilibriumbetweensolid and gasphases.

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    TRANSITIONSBETWEEN PHASES

    As P and T increase, you finally reach the

    CRITICAL T and P

    .

    LIQUID

    GAS

    Pcritical

    HighPr

    essure

    High Temperature

    Tcritical

    Note that linegoes straight up

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    Copyright (c) 1999 by Harcourt Brace & Company

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    TRANSITIONSBETWEEN PHASES

    .

    LIQUID

    GAS

    Pcritical

    HighPr

    essure

    High Temperature

    Tcritical

    Note that linegoes straight up

    Above critical T

    no liquid exists

    no matter how

    high the

    pressure.

    As P and T increase, you finally reach the

    CRITICAL T and P

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    Critical T and P

    COMPD Tc(oC) Pc(atm)H2O 374 218

    CO2 31 73

    CH4 -82 46Freon-12 112 41

    (CCl2F2)

    Notice that Tc and Pc depend onintermolecular forces.

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    Solid-Liquid EquilibriaIn any system, if you increase P the DENSITY

    will go up.

    Therefore as P goes up, equilibrium favors

    phase with the larger density (orSMALLER

    volume/gram).Liquid H2O Solid H2O

    Density 1 g/cm3 0.917 g/cm3

    cm3/gram 1 1.09

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    Copyright (c) 1999 by Harcourt Brace & Company

    All rights reserved

    Solid-Liquid EquilibriaIn any system, if you increase P the DENSITY

    will go up.

    Therefore as P goes up, equilibrium favors

    phase with the larger density (orSMALLER

    volume/gram).Liquid H2O Solid H2O

    Density 1 g/cm3 0.917 g/cm3

    cm3/gram 1 1.09LIQUID H2OICE

    favored atlow P

    favored athigh P

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    Solid-Liquid Equilibria

    SolidH2O

    LiquidH2O

    P

    T

    760mmHg

    0 C

    Normalfreezingpoint

    LIQUID H2OICEfavored atlow P

    favored athigh P

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    Solid-Liquid Equilbria

    Raising the pressure at

    constant T causes

    water to melt.

    The NEGATIVE SLOPEof the S/L line is

    unique to H2O.

    Almost everything

    else has positiveslope.

    P

    T

    freezingSolidH2O

    LiquidH2O

    760mmHg

    0 C

    Normal

    point

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    Solid-Liquid

    Equilbria

    The behavior of water

    under pressure is an

    example ofLE CHATELIERS

    PRINCIPLE

    At Solid/Liquidequilibrium, raising P

    squeezes the solid.

    It responds by going to

    phase with greaterdensity, i.e., the liquid

    phase.

    Solid

    H2O

    LiquidH2O

    P

    T

    760mmHg

    0 C

    Normalfreezingpoint

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    Solid-Vapor Equilibrium

    At P < 4.58 mmHg and T < 0.0098 C

    solid H2O can go directly to vapor. This

    process is called SUBLIMATION

    This is how a frost-free refrigerator works.