
the same conditions exist in most sections of the reactor, the conditions near the
reactor inlet and near the reactor wall are different from those in the remainder
of the reactor. Since these zones usually represent a small portion of the reactor,
the CSTR model provides a reasonable description of the well-agitated large reac-
tors. Figure 8.1 shows schematically a liquid-phase CSTR.
8.1 DESIGN EQUATIONS AND AUXILIARY RELATIONS
The design equation of a CSTR was derived in Chapter 4. The design equation,
written for the mth-independent reaction is
Z
m
out
Z
m
in
¼ r
m
out
þ
X
n
D
k
a
km
r
k
out
!
t
t
cr
C
0
(8:1:1)
where Z
m
is the dimensionless extent of the mth-independent reaction, defined by
Eq. 2.7.2:
Z
m
¼
_
X
m
(F
tot
)
0
(8:1:2)
and t is the dimensionless space time of the reactor defined by Eq. 4.4.8:
t ¼
V
R
v
0
t
cr
(8:1:3)
where t
cr
is a conveniently selected characteristic reaction time (defined
by Eq. 3.5.1), and C
0
is a conveniently selected reference concentration
defined by
C
0
¼
(F
tot
)
0
v
0
(8:1:4)
where (F
tot
)
0
and v
0
are, respectively, the total molar flow rate and the volumetric
flow rate of the reference stream.
As discussed in Chapter 4, to describe the operation of a CSTR with multiple
reactions, we have to write Eq. 8.1.1 for each independent chemical reaction.
The solution of the design equations (the relationships between Z
m
out
’s and t )pro-
vide the reaction operating curves and describe the reactor operation. To solve the
design equations, we have to express the rates of the chemical reactions that take
place in the reactor in terms of Z
m
’s and t. Below, we derive the auxiliary relations
used in the design equations.
The volume-based rate expression of the ith chemical reaction (Eq. 3.3.1 and
Eq. 3.3.6) is
r
i
¼ k
i
(T
0
)e
g
i
(u1)=u
h
i
(C
j
,
s) (8:1:5)
318 CONTINUOUS STIRRED-TANK REACTOR