Biomedical Engineering Reference
In-Depth Information
In general, it can be shown that the solution for
q
P
in Eq. (8.14) is
0
1
e
K
1
ðabÞ
t
b 1
@
A
u
ð
t
Þ
q
P
¼
ð
8
:
21
Þ
b
a
e
K
1
ðabÞ
t
1
where
s
2
Þ þ
K
2
K
1
l
¼
ð
q
A
ð
0
Þþ
q
B
ð
0
Þþ
2
q
P
ð
0
Þ
4
ð
q
A
ð
0
Þþ
q
P
ð
0
Þ
Þ
q
B
ð
ð
0
Þþ
q
P
ð
0
Þ
Þ
Þþ
K
2
K
q
A
ð
0
Þþ
q
B
ð
0
Þþ
2
q
P
ð
0
1
þ
l
a
¼
2
Þþ
K
2
K
q
A
ð
0
Þþ
q
B
ð
0
Þþ
2
q
P
ð
0
1
l
b
¼
2
Next, consider the case in which
q
B
ð
0
Þ
q
A
ð
0
Þ
, where the change in
q
B
is small and can
be treated as a constant
q
B
ð
0
Þ:
Thus, an approximation for Eq. (8.14) is
q
P
¼
K
q
B
ð
0
Þ
q
A
K
1
q
P
ð
8
:
22
Þ
1
Next, we remove
q
A
in Eq. (8.22) by letting
q
A
¼
q
P
ð
0
Þþ
q
A
ð
0
Þ
q
P
, giving
q
P
¼
K
q
B
ð
0
Þ
q
A
ð
ð
0
Þþ
q
P
ð
0
Þ
Þ
K
ð
q
B
ð
0
Þþ
K
1
Þ
q
P
ð
8
:
23
Þ
1
1
which can be straightforwardly solved as
ð
K
1
q
P
ð
0
Þ
K
q
B
ð
0
Þ
q
A
ð
0
Þ
Þ
þ
K
ð
q
B
ð
0
Þ
q
A
ð
ð
0
Þþ
q
P
ð
0
Þ
Þ
Þ
1
1
e
K
1
q
B
ð0Þþ
K
1
ð
Þ
t
q
P
¼
u
ð
t
Þ
ð
8
:
24
Þ
ð
K
q
B
ð
0
Þþ
K
1
Þ
ð
K
q
B
ð
0
Þþ
K
1
Þ
1
1
8.1.4 Higher-Order Chemical Reactions and Sequential Reactions
Consider the higher-order chemical reaction in Eq. (8.25):
ð
8
:
25
Þ
in which a
A
of reactant
A
and b
B
of reactant
B
form product
P,
and
P
has a reverse reaction
to form a
A
þ
b
B.
The law of mass action for Eq. (8.25) is
b
B
K
1
q
P
a
q
P
¼
K
1
q
A
q
b
B
þ
K
1
q
P
a
q
A
¼
K
1
q
A
q
ð
8
:
26
Þ
b
B
þ
K
1
a
q
B
¼
K
q
A
q
q
P
1