Biomedical Engineering Reference
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K
1
S
K
B
C
B
q
A
¼ K
1
q
B
¼
(9.109)
S
þ K
B
C
B
þ K
1
1
S
K
B
C
B
Substituting
Eqns (9.107) and (9.109) into (9.100)
, we obtain
k
A
C
A
k
A
K
1
C
A
k
A
k
A
K
1
S
K
B
C
B
S
K
B
C
B
r ¼ C
s
S
K
B
C
B
¼ k
A
C
s
(9.110)
þ K
B
C
B
þ K
1
þ K
B
C
B
þ K
1
1
1
S
K
B
C
B
At equilibrium,
r
¼
0, we have
C
B;eq
C
A;eq
¼
1
k
A
k
A
K
1
K
eq
¼
(9.111)
S
K
B
also noting that
k
A
k
A
K
A
¼
(9.112)
we have
K
S
K
A
K
B
K
eq
¼
(9.113)
Eqn
(9.110)
can be rewritten as
C
A
K
1
eq
C
B
r ¼ k
A
C
s
(9.114)
þ K
B
C
B
þ K
1
1
eq
K
A
C
B
Eqn
(9.114)
can also be written as
C
A
K
1
eq
C
B
r ¼ k
A
C
s
(9.115)
þ K
B
C
B
þ K
A
C
A
1
By noting that
C
A
¼ K
1
eq
C
B
(9.116)
as the equilibrium constant is not dependent on the nature of the surfaces.
C
A
is the virtual or
equilibrium concentration of A in the bulk fluid phase with the surface overage. This is deriv-
able because the concentration of A on the surface is in equilibrium with other components
(or species) in the system as the rest of the steps that govern the overall reaction are fast equi-
librium steps. One can observe from
Table 9.3
that it holds true for all other cases. Comparing
Eqn (9.115)
with
Eqn (9.110)
, we note that
1
q ¼
(9.117)
þ K
B
C
B
þ K
A
C
A
1
and
K
A
C
A
q
A
¼
(9.118)
þ K
B
C
B
þ K
A
C
A
1
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