12. condensation

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    12. CONDENSATION

    Similar to natural (free) convection

    But with phase change steam (vapor) to liquid

    Liquid film or drops that form by condensation movesalways naturally downwards the role of gravitation

    Takes place where the surface temperature is below

    the saturation temperature Two modes film and dropwise condensation

    Under what conditions

    the dropwise condensation

    can be reached and

    maintained?

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    Regardless of the condensation mode, the condensate

    creates a resistance to heat transfer between the

    vapor and the surface Resistance increases with condensate thickness

    How to avoid an increase in condensate thickness?

    Dropwise condensation is superior to film condensation

    Various surfactants used to inhibit wetting (teflon,

    silicon, waxes, fatty acids etc.) Coatings gradually lose their effectiveness fouling,

    oxidation film condensation occurs

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    Laminar film condensation on a vertical wall

    2

    2

    f y

    ugdx

    dp

    1

    y

    uvx

    uu

    ++=

    +

    The same momentum PDE as for the natural convection

    (gravitation in + x direction):

    0p =No movement iny - direction

    xp Same in the condensate filmand in the vapor

    gp

    v

    =

    Pressure difference results fromthe weight of the fluid column

    2

    2

    f

    v

    y

    ug

    1

    y

    uv

    dx

    uu

    +

    =

    +

    x

    y

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    Laminar film condensation on a vertical wall

    Assumption:

    Momentum and energy transfer by advection in the film is

    negligible what does it mean?

    2

    2

    y

    Ta

    y

    Tv

    x

    Tu

    =

    +

    Energy PDE:

    Momentum PDE:2

    2

    f

    v

    y

    ug

    1y

    uvdx

    uu+

    =+

    2

    2

    yTa

    yTv

    xTu

    =

    +

    Energy PDE:

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    x

    y

    Laminar film condensation on a vertical wall

    Momentum equation:

    0g

    dy

    ud vf2

    2

    =

    + y0,y

    u == at

    B.C.: u=0 at y=0

    Solution:

    21vf

    CyC2

    gu ++= ( )

    =

    22vf

    y

    y22

    gu

    Energy equation:

    0dy

    Td2

    2

    =B.C.: T=T

    w

    at y=0

    T=Tsat at y=

    21CyCT +=

    ( ) y

    TTTT wsatw +=

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    Laminar film condensation on a vertical wall

    In both equations unknown condensate film thickness .

    How to determine it? And how it develops along the surface?

    Lets express the condensate mass flow in the film:

    =)(

    )(x

    0fudyxm&

    ( )

    =22

    vf

    y

    y2

    2

    gu

    3vf3vff

    3

    g

    3

    gm

    =

    =&

    ( )d

    g

    dx

    d

    mdx

    x

    mmd

    2vf

    =

    =

    =

    &&&

    Net inflow of condensate into the film:

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    Laminar film condensation on a vertical wall

    This inflow of condensate into the film is due to the release of

    latent heat from the vapor:

    mdlQd 23 && =

    This heat transfer rate (tepeln tok) is transferred through the

    condensate film by conduction:

    mdldx.1

    TTQd 23

    wsat && =

    =

    ( ) dxTTl

    1

    md wsat

    23

    =&

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    Laminar film condensation on a vertical wall

    ( )d

    gmd

    2vf

    =& from mass balance

    ( ) dxTTl1

    md wsat

    23=& from energy balance

    ( )( )dxTT

    l

    1

    d

    gwsat

    23

    2vf

    =

    Equation for the condensate film thickness:

    B.C.: = 0 atx= 0

    ( )( )

    41

    vf23

    wsat

    gl

    xTT4

    =

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    x

    y

    Heat transfer coefficient

    ( )wsatx0y TTdy

    dTq == =&

    Determine on the basis of the equality of latent heat transfer

    by conduction and convection across the condensate film:

    Linear temperature profile across the film

    ( )( )wsatx

    wsat TT

    TT=

    ( )( )

    41

    wsat

    3vf23

    xxTT4

    gl

    ==

    Try to analyze the influence of

    major parameters on x

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    Heat transfer coefficient

    Local Nusselt number:

    Average heat transfer coefficient on the wall

    of the height L :

    x

    y

    ( )( )

    41

    wsat

    3vf23x

    x TT

    xgl

    0,707

    x

    Nu

    =

    L

    L

    0x

    3

    4dx

    L

    1 ==

    Average Nusselt number:

    ( )

    ( )

    41

    wsat

    3vf23

    L

    TT

    Lgl0,9428

    LNu

    =

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    Heat transfer coefficient

    Or in a different form:

    ( )

    41

    III.

    wsatp

    23

    II.

    pf

    I.

    f

    vf2

    3

    LTTc

    l

    c

    gL0.9428Nu

    =44 344 2132144 344 21

    I Archimedes number

    II Prandtl number

    III - Jacob (or K) number

    ( ) 41L KPrAr0,9428Nu =

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    Heat transfer coefficient

    Experiments reveal that heat transfer more intensive than

    predicted from the theory. Why?

    Condensate film waves and the film isthus thinner - lower thermal resistance

    higher heat transfer

    ( ) 41L KPrAr1,13Nu =

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    Heat transfer coefficient on horizontal tubes

    Height of the wall is replaced by the diameter of the

    tube and the constant is lower:

    ( )( )

    41

    wsat

    3

    vf23d TT

    dgl0,729Nu

    =

    An obvious question:

    Whats better for the condensation?

    Horizontal or vertical tube?