Numerical Analysis of Simultaneous Heat and Mass

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  • 7/23/2019 Numerical Analysis of Simultaneous Heat and Mass

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    Numerical analysis of simultaneousheat and mass transfer during

    absorption of polluted gases bycloud droplets

    T. Elperin, A. Fominykh and B. Krasovitov

    Department of Mechanical EngineeringThe Pearlstone Center for Aeronautical Engineering

    StudiesBen-Gurion Universit of the !egev

    P"#"B" $%&' Beer Sheva ()*+%' ,SAE.

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    Motivation and goals

    Description of the model

    Results and discussion

    Conclusions

    Outline of the presentation

    Ben-Gurion University of the Negev

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    Effect of vapor condensation at the surface of stagnant droplets on therate of mass transfer during gas absorption by growing droplets:

    uniform temperature distribution in both phases was assumed (seee.g., Karamchandani, P., Ray, A. K. and as, !., "#$%&'

    liuid)phase controlled mass transfer during absorption wasinvestigated when the system consisted of liuid droplet, its vapor

    and solvable gas (see e.g., Ray A. K., *uc+aby . -. and hah /.,"#$0, "#$#&'

    1as absorption by falling droplets accompanied by subseuentdissociation reaction (see e.g., 2aboolal et al. ("#$"&, 3alce+ andPruppacher ("#$%&, Ale4androva et al., 566%&'

    imultaneous heat and mass transfer during droplet evaporation orgrowth:

    model of physical absorption (Elperin et al., 5667&'

    model ta+ing into account subseuent dissociation reaction (Elperinet. al, 5660&.

    Gas absorption by cloud droplets: Scientific background

    Ben-Gurion University of the Negev

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    Gas-liquid

    interface

    Droplet

    Absorption equilibria

    Ben-Gurion University of the Negev

    =pollutant molecule

    =pollutant captured in solution

    Air

    SO2

    Aqueous phase sulfur dioxide/water

    chemical equilibria

    is the species in dissolved state

    *enry8s -aw:

    Electro neutrality euation:

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    Description of the model

    Ben-Gurion University of the Negev

    Governing equations

    1. gaseous phaser>R (t)

    ( ) 022 =

    +

    rrrt

    r v

    ( ) ( )

    =

    +

    r

    YrD

    rYr

    rY

    tr

    jjjrj

    222 v

    ( )

    =

    +

    r

    Trk

    rTcr

    rt

    Tcr eeepr

    ep 222v

    2. liquid phase0 < r

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    Description of the model

    Ben-Gurion University of the Negev

    ( )

    + ===

    =

    =Rr

    A

    Rr

    AAsARrA r

    YD

    r

    YDYj

    L

    LL v

    #he $o%iui%& $odi%io 'or %he radial 'lu o' %he asora%e a% %he drople%sur'a$e reads*

    O%her o+solule $opoe%s o' %he ier% adi%ures are o% asored i %he

    liquid

    AjjjRJ jj == ,1,042

    (-)

    ()

    #a/ig i%o a$$ou% !q. () ad usig aelas%i$ approia%io

    e $a o%ai %he epressio 'or S%e'a elo$i%&*

    ( )

    ( )

    ( )+ ==

    =

    RrRr

    As

    r

    Y

    Y

    D

    r

    Y

    Y

    D L

    LL 1

    1

    1

    1 11

    v ()

    here sus$rip% 91deo%es a%er apor spe$ies

    ( ) 02 =

    rrr

    v

    Stefan velocity and droplet vaporization rate

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    Description of the model

    Ben-Gurion University of the Negev

    #he a%erial ala$e a% %he gas+liquid i%er'a$e &ields*

    ( )( )RtRRtd

    mds

    L = ,4 2 v ()

    #he assuig e o%ai %he 'olloig epressios 'or %hera%e o' $hage o' drople%s radius*

    ( )

    ( )

    ( )+ ==

    +

    =

    RrRr

    A

    r

    Y

    Y

    D

    r

    Y

    Y

    DR

    L

    L

    L 1

    1

    1

    1 11

    (10)

    >>L

    Stefan velocity and droplet vaporization rate

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    Description of the model

    Ben-Gurion University of the Negev

    Stefan velocity and droplet vaporization rate

    ( )+=

    =

    Rr

    sr

    Y

    Y

    D 1

    1

    1

    1v

    ( ) +=

    =

    Rrr

    Y

    Y

    DR

    L

    1

    1

    1

    1

    ( ) +=

    = Rrs rY

    Y

    D 1

    1

    1

    1v

    ( )+=

    =

    Rrr

    Y

    Y

    DR

    L

    1

    1

    1

    1

    ( )

    ( )

    =

    Rr

    A

    r

    Y

    Y

    D L

    LL

    11

    ( )

    ( )

    +

    =Rr

    A

    r

    Y

    Y

    D L

    L

    11

    I %he $ase he all o' %he ier%

    adi%ures are o% asored i

    liquid %he epressios 'or S%e'a

    elo$i%& ad ra%e o' $hage o'

    drople% radius read

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    Description of the model

    Ben-Gurion University of the Negev

    Initial and boundary conditions

    #he ii%ial $odi%ios 'or %he s&s%e o' equa%ios (1)(5) read*

    A% % 6 0, *0 0Rr ( ) ( )LL TT 0=

    ( ) ( )LLAA YY 0,=

    A% % 6 0, *0Rr ( )rYY jj 0,= ( )rTT ee 0,=(11)

    A% %he drople% sur'a$e*

    sj

    Rr

    jj Y

    r

    YD v =

    +=

    (12)

    (13)

    ( ) ( )

    + ===

    =+

    Rr

    Aa

    Rr

    v

    Rr

    ee

    r

    YDL

    r

    Tk

    td

    RdL

    r

    Tk

    L

    LL

    L

    LL (14)

    ( )

    + ==

    =

    Rr

    A

    Rr

    AAsA

    r

    YD

    r

    YDY

    L

    LL v

    ( )

    +=

    RRe

    LTT (15)

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    Description of the model

    Ben-Gurion University of the Negev

    Initial and boundary conditions

    #he equiliriu e%ee solale gaseous ad dissoled i liquid spe$ies$a e epressed usig %he 7er&s la

    (1-)

    here

    (1)

    I %he $e%er o' %he drople% s&e%r& $odi%ios &ields*

    (1)

    (1)

    ( )[ ] ASA pHSC8

    )I"(I" ==

    ( )

    0

    0

    =

    =rr

    T L ( )

    0

    0

    =

    =r

    A

    r

    Y L

    A% ad %he ;so'%8oudar& $odi%ios a% i'ii%& are iposed0>t r

    0=

    r

    j

    r

    Y0=

    r

    e

    r

    T

    [ ] [ ]

    ++= ++ 22118

    )I"( 12H

    KK

    H

    KHH SOS

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    Spa%ial $oordia%e %ras'ora%io*

    #he gas+liquid i%er'a$e is lo$a%ed a% 9oordia%esxad w$a e %rea%ed ide%i$all& i

    ueri$al $al$ula%ios;

    #ie ariale %ras'ora%io*

    #he s&s%e o' oliear paraoli$ par%ial di''ere%ial equa%ios (1)(5) assoled usig %he e%hod o' lies;

    #he esh poi%s are spa$ed adap%iel& usig %he 'olloig 'orula*

    Method of numerical solution

    Ben-Gurion University of the Negev

    ( ),1

    tRrx = ( );0'or tRr

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    Results and discussion

    Ben-Gurion University of the Negev

    Aerage $o$e%ra%io o' %he

    asored SO2

    i %he drople%*

    Figure 1.:epede$e o' aerage aqueous

    sul'ur dioide olar $o$e%ra%io s. %ie

    'or arious alues o' rela%ie huidi%&.

    Figure 2.:epede$e o' diesioless aerage

    aqueous SO2 $o$e%ra%io s. %ie 'or arious

    ii%ial sies o' eapora%ig drople%R0.

    rela%ie asora%e $o$e%ra%io

    is de%eried as 'ollos*

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    Results and discussion

    Ben-Gurion University of the Negev

    Figure 3.:rople% sur'a$e %epera%ure s. %ie

    (#06 2 , #=6 23 , 7 6 0?).

    Figure 4.!''e$% o' S%e'a 'lo ad hea% o'

    asorp%io o drople% sur'a$e %epera%ure

    (!lperi e% al. 2005).

    Figure 5.:rople% sur'a$e %epera%ure s. %ie*

    1 odel %a/ig i%o a$$ou% %he equiliriudisso$ia%io rea$%ios; 2 odel o' ph&si$al

    asorp%io.

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    Results and discussion

    Ben-Gurion University of the Negev

    Figure 7.Aerage $o$e%ra%io o' aqueous

    sul'ur spe$ies ad %heir su s. %ie ( 7 6101?).

    Figure 6.Aerage $o$e%ra%io o' aqueous

    sul'ur spe$ies ad %heir su s. %ie ( 7 6

    0?).

    pHis a easure o' %he a$idi%&

    or al/alii%& o' a solu%io.

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    Results and discussion: the interrelation beteenheat and mass transport

    Ben-Gurion University of the Negev

    Decreases Stefan

    velocity

    Absorption during

    droplet evaporation

    Diffusion of

    absorbate

    hermal effect of

    absorption

    Reactions of

    dissociation

    Decreases vapor flu!

    "ncreases droplet surface

    temperature

    "ncreases

    vapor flu!

    Decreases effective

    #enry$s constant

    Decreases droplet

    surface temperature

    "ncreases absorbate

    flu!

    "ncreases effective

    #enry$s constant

    Decreases absorbate

    flu!

    "ncreases Stefan

    velocity

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    !onclusion

    Ben-Gurion University of the Negev

    #he o%aied resul%s sho, %ha% %he hea% ad ass %ras'er ra%es i a%erdrople%+air+a%er apor s&s%e a% shor% %ies are $osideral& eha$eduder %he e''e$%s o' S%e'a 'lo, hea% o' asorp%io ad disso$ia%io rea$%iosi%hi %he drople%.

    I% as sho %ha% olieari%& o' %he depede$e o' drople% sur'a$e%epera%ure s. %ie s%es 'ro %he i%era$%io o' di''ere% pheoea.

    @ueri$al aal&sis shoed %ha% i %he $ase o' sall $o$e%ra%ios o' SO2ia gaseous phase %he e''e$%s o' S%e'a 'lo ad hea% o' asorp%io o %hedrople% sur'a$e %epera%ure $a e egle$%ed.

    #he deeloped odel allos %o $al$ula%e %he alue o' p7 s. %ie 'or o%heapora%ig ad groig drople%s. #he per'ored $al$ula%ios shoed %ha%%he depede$e o' p7 i$rease i%h %he i$reasig rela%ie huidi%& (7).

    #he per'ored aal&sis o' gas asorp%io & liquid drople%s a$$opaied &drople%s eapora%io ad apor $odesa%io o %he sur'a$e o' liquid drople%s$a e used i $al$ula%ios o' s$aegig o' haardous gases i a%osphere& rai, a%ospheri$ $loud eolu%io.