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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