Environmental Engineering Reference
In-Depth Information
Δ
z
F
j
0
F
j
F
j
(
z
)
F
j
(
z
+
Δ
z
)
FIGURE 6.3
Schematic of a tubular or plug-flow reactor.
Taking the limit as
Δ
z
→
0 and rewriting, we obtain
1
A
c
d
F
j
d
z
=
v
j
r
(6.11)
or
d
F
j
d
V
=
v
j
r
.
(6.12)
It can be shown that the above equation also applies to the case where the cross-
sectional area varies along the length of the reactor. This is the case of a river going
through several narrow channels along its path.
If the reaction is first order, namely, A
→
B, the rate of disappearance of A is
r
=
kC
A
. The stoichiometry of the reaction is such that
ν
A
=−
1. If we consider a
constant-density reactor, and note that
F
A
=
Q
0
C
A
with
Q
0
being the volumetric flow
rate, we have
d
C
A
d
V
=
k
Q
0
−
C
A
.
(6.13)
Integrating with the initial condition,
C
A
=
C
A0
at 0, we obtain
k
ln
C
A0
Q
0
V
=
(6.14)
C
A
If 50% of
C
A0
has to be converted into products, then
V
=
0.693
Q
0
/k
is the reactor
volume required.
6.1.1.4
Design Equations for CSTR and PFR
For any general stoichiometric equation of the form
a
A
+
b
B
→
c
C
+
d
D, we can
write the following equation on a per mole of A basis:
b
a
B
c
a
C
d
a
D.
A
+
−→
+
(6.15)
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