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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" $%&' Beer Sheva ()*+%' ,SAE.
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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Motivation and goals
Description of the model
Results and discussion
Conclusions
Outline of the presentation
Ben-Gurion University of the Negev
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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Effect of vapor condensation at the surface of stagnant droplets on therate of mass transfer during gas absorption by growing droplets:
uniform temperature distribution in both phases was assumed (seee.g., Karamchandani, P., Ray, A. K. and as, !., "#$%&'
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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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:
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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)
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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*
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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.
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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
7/23/2019 Numerical Analysis of Simultaneous Heat and Mass
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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.