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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