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10 MassTran

Date post: 04-Jun-2018
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    Dimensionless Groups

    Shi ji j

    i j

    k d

    ,

    ,

    ,

    Sc i ji j

    ,

    ,

    Revd

    Sherwood number

    Reynolds number

    Schmidt number

    mass transfer

    fluid flow

    mixture property

    diameter

    film thickness

    Re 1 laminarRe 1 turbulent

    Sc 1 in gasesSc 103 in liquids

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    Heat Transfer

    mass transfer heat transfer

    )Sc(Re,Sh f )Pr(Re,Nu f

    k h

    a

    same as

    replace thermal diffusivity

    )( pca

    by

    by

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    Tubes - laminar

    z

    d

    vd

    1

    20

    v

    d

    inlet zone fully developed

    concentration of absorbing species

    laminar Re 2000

    Sh Sci j i j z

    d, ,. Re

    162 1 3 1 31 3

    Shi j, .3 66

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    Tubes - turbulent

    v

    d

    turbulent

    inlet zone(short) fully developed

    Re 2000 Sh Sci j i j d

    z, ,. . Re

    0 027 1 0 7 4 5 1 3

    inlet correction

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    Membrane Spacer

    d

    zv

    Sh Sci j i j d

    z, ,. Re

    19 1 2 1 3

    1 2

    membranes

    spacer wires

    300 2000 Re

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    Packed Beds

    superficial velocity v void fraction e particle diameter d

    external (film) coefficient Sh Sci j i,j ,.

    Re0 34 2 3 1 3

    e

    minimum value (chromatography) Shi j, 4

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    Packing with Gas

    and Liquid

    liquid as a film

    over the packing

    gas through and

    around the packing

    liquid, superficial velocity vL

    gas, superficial velocity vG

    d

    Sh Re Sc2 3

    i,j

    G G

    i,j

    G 0 9 1 1 3 1 3

    . e

    e void fraction

    Sh Re Sc1 2

    i,j

    L L

    i,j

    L 19 1 3

    liquid:

    gas:

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    outside Rigid Interfaces

    k g i j i j , ,

    /

    .

    0 3 21 3

    , ,and i j are values in the fluid outside

    for short times

    for small particles

    for large particles

    boundary layer theory

    k

    ti j

    i j

    ,

    ,. 113

    k

    di j

    i j

    ,

    ,2

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    surface active agents

    swept to the back

    these immobilise the

    drop or bubble whend

    f

    g

    1 2/

    fis the fouling (fudge) factor

    f0 2. in clean liquidsf 1 in dirty liquids

    the transition is atd 1 mm

    cause surface tension

    gradients d

    Mobile or Rigid?

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    Bubbles with Mobile Interfaces

    bubbles:

    k g i j i j , ,

    /

    . 0 4

    2 2

    3

    1 6

    and are for the liquid (outside)

    outside

    k g i jd i jd, ,

    /

    . 0 4

    2 23

    1 6

    inside (?)

    i jd

    ,

    i j,

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    Mobile Drops in a Liquid

    i jd

    ,

    i j,

    d

    mobile drops in a liquid

    calculate the rigid and mobile

    (bubble) coefficients separately

    interpolate using d

    k k ki j i j mobile

    i j

    rigid

    , , ,

    .

    .

    .

    1

    1 0 3

    0 3

    1 0 3

    (these differ for the outerand

    innercoefficients)

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    Drops in a Gas

    dg

    2

    1 2

    /

    dg

    4

    1 2

    /

    rigid

    sphere mobile oscillating drop drop shatters


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