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
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