Environmental Engineering Reference
In-Depth Information
is the mass of pollutant per unit bed weight. The general Freundlich isotherm (see
Chapter 3) in the following form is found to best fit the data over a wide range of
concentrations for activated carbon:
[
1 /n
] F
K Freun
A
W 0 =
.
(6.149)
Hence
V g
ρ ads
K 1 /n
( 1
( 1 /n))
V ads =
Freun [
A
]
,
(6.150)
F
where V g =
ρ g A c is the superficial gas velocity.
Consider a differential volume of the bed A c d x .A material balance on the pollutant
gives the following:
M F /
input by flow
=
output by flow
+
mass gained on the bed by transfer from gas to solid.
G F [
A
]=
G F (
[
A
]+
d
[
A
]
)
+
K mt A C (
[
A
]−[
A
] eq ) d x ,
(6.151)
where [A] eq is the equilibrium value of air concentration that would correspond to the
actual adsorbed concentration W in the differential volume. K mt is the overall mass
transfer coefficient (time 1 ) from gas to solid. Rearranging, we obtain
K Freun W n ) d x .
V g d
[
A
]=
K mt (
[
A
]−
(6.152)
[
]=[
] F at x
=
Rearranging and integrating using the boundary conditions that
A
A
0
and
[
A
]=
0at x
= δ
,
δ
V g
K mt
0
d
[
A
]
d x
=−
K Freun W n ) .
(6.153)
(
[
A
]−
A ] F
0
[
An overall mass balance over the differential volume gives [A] G F =
A c W
ρ ads V ads .
n [A] 1 n
F
Utilizing the expression for v ad and rearranging, we obtain K Freun W n
=[
A
]
.
Hence,
V g
K mt
0
d
[
A
]
δ =−
F
.
(6.154)
1 /n
n
[
A
]−[
A
]
[
A
]
A ] F
[
Note that as K mt →∞
0 and the process becomes equilibrium controlled.
Utilizing the dimensionless variable
,
δ →
η =[
A
] / [
A
] F and K mt δ /V g = St , the Stanton
number , we can write
1
η
η − η
d
=
St
n .
(6.155)
0
 
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