Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras
Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras
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Transcript of Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras
Dr. R. Nagarajan
Professor
Dept of Chemical Engineering
IIT Madras
Advanced Transport PhenomenaModule 6 Lecture 29
1
Mass Transport: Illustrative Problems
Mass Transport: Illustrative Problems
2
SOLUTION TO THE PROBLEM
3
4
SOLUTION
Catalytic Converter
a. Mechanism of CO(g) transport to the wall
If Re < 2100 (see below),transport to the wall is by
Fick diffusion of CO(g) through the prevailing
mixture.2
1.73 20.216.
300CO mix CO N
T cmD D
p s
SOLUTION
5
Therefore
Analogous heat transfer diffusivity is for gas
mixture
b. Discuss whether the Mass transfer Analogy Conditions(M A
C) and Heat transfer Analogy Conditions (H A C) are met;
implications ?
Since Mmix and Mco are close hence we will
assume
; CO COy
, 1 0.02. CO
SOLUTION
pk c
1.73 20.216 600
600 ,1 0.684 .1 300CO mix
cmD K atm
s
6
c. Sc for the mixture :
Now:
and:
CO mix CO mixSc v D
1700 500
2mix air
43.31 10 poise
43
1 28.975.88 10
82.06 600
pM g
RT cm
SOLUTION
7
therefore
therefore
2
0.563mix
cmv
s
0.5630.823
0.684CO mixSc v D
SOLUTION
8
d. L=? We will need Re
Now:
therefore (laminar-flow regime)
4 0.15 0.1540.15
4 0.15
eff
cm cmAd cm
P cm
310U cm s20.562 v cm s
310 0.15Re 267
0.562
SOLUTION
9
For a square channel
and (used below).
If then the mass-transfer analogy is:
2.976 mNu Re 14.227 . fC
, 0,CO w
,
,
exp 40
.
CO b
mmCO b
zF entrance Nu
SOLUTION
10
where
We estimate at which
If
then
1.
Re .
meff
z
Sc d
z L 0 0.05. b bL
0.05 exp X
SOLUTION
1ln 2.9957
0.05 = X
11
therefore
Tentatively, assume F (entrance =1).Then:
that is,
(at which F (entrance) is indeed ). Solving for L gives: L
=8.3 cm ( needed to give 95 % CO-Conversion).
4 . . 2.9957. m mNu F entrance
01
4 . . 2.976 2.9957;267 0.823 0.15
L
cm
SOLUTION
0 2.9957
0.251664 2.976
m
1
12
e. Discuss underlying assumptions, e.g.,
fully developed flow?
nearly constant thermo physical properties?
no homogeneous chemical reaction?
“ diffusion-controlled” surface reaction?
f. If the catalyst were “ poisoned,” it would not be able to maintain
. This would cause to exceed 8.3 cm. If catalyst
were completely deactivated, then and, of course, , ,CO w CO b
, , ,CO w CO b
SOLUTION
reqL
reqL
13
g. If the heat of combustion is 67.8 kcal/mole CO, how much
heat is delivered to the catalyst channel per unit time?
Overall CO balance gives the CO-consumption
rate/channel:
where
, , 1 . ,CO channel COm m conversion
24 3
2
5.04 10 10 0.15
1.13 10 .
=
m U A
g s per channel
SOLUTION
14
Moreover,
hence,
and
, 1 0.02; 0.95; CO Conversion
2,
4
1.13 10 0.02 0.95
2.156 10
=
CO channelm g s
g s
3167.8 . 2.42 10
28
kcal g mole CO calQ
g mole CO g g
SOLUTION
15
Therefore
The “sensible” heat transfer required to keep the wall
at 500 K can be calculated from a heat balance on the
8.3 cm-long duct- i.e., once we calculate , we
have :
4 32.156 10 2.42 10 0.522 . CO oxid
cal calQ
g s
bT L
0 , - sensible p b bQ m c T T L
SOLUTION
16
where
Mixing cup avg temp at duct outlet ?
21.13 10 ,
0.251
0 700 .
p
b
m g s
c cal g K
T K
exp 4 . . .
0
w b
h hw b
T T LNu F entrance
T T
SOLUTION
17
Again, we see that
Moreover,
1 since;F entrance
1 1 8.3
. ,Re.Pr 267 0.706 0.15
0.293.
heff
h
L
d
2.976;mNu
SOLUTION
18
therefore
and
exp -4 0.293 2.976 0.0304; 0
b w
b w
T L T
T T
5000 0304
700 500506
. ,
=
b
b
T Lor
T L K
SOLUTION
19
Therefore,
2
0
1 135 10 0 251 700 506
.
= . ..
sensible p b bQ m c T T L
g calK
s g K
0 552
0 522 0 552
1 07
.
., . ,
. .
= . .
sens
total CO oxid sens
ie Q cal s
Q Q Q
calper channel
s
SOLUTION
20
h. “Quasi-Steady” Application of These Results? Note that:
and
hence, if the characteristic period of the unsteadiness >> 8.2 ms, the previous results can be used at each flow condition.
flow 3
2 2
diff 2CO mix
L 8 3t 8 3 ms
U 10 cm s
w 2 0 15 2t 8 2 ms
cmD0 684
s
..
.. ;
.
SOLUTION
21
i. Pressure Drop
We have:
Therefore
?p
2
14 227 for square duct, laminar flow.
1 Re2
.wfC
U
21 14 227
2 Re
.. ,w U perimeter mean shear stress
SOLUTION
22
But
Therefore
242 3 2
3 2
1 5 043 1010 =2.98 10 .
2 2
. g cm dyneU
cm s cm
2 2 3
2
14 222 98 10 2 98 10 5 335 10
267
1 345
.( . ) . .
. .
f
w
C
w dyne cm
SOLUTION
23
From overall momentum balance:
4 4 0 15 ( . )w cm
2 2
5 1
. . .
- = 4
= 1.345 4 8.3 0.15 2.48 10
- = 2.93 10 0.003%.
duct channel w
w
p A Perim L
p L w
dyne cm
p p
SOLUTION
24