Biomedical Engineering Reference
In-Depth Information
where W s is the shaft work exported out of the reaction mixture, which is the negative of the
stirrer output, and
Q is the heat transfer into the reaction mixture. That is,
Q ¼ UA H T c T
(5.96)
where U is the overall heat-transfer coefficient and A H is the total heat transfer area.
Substituting into Eqn (5.95) , we obtain
X
F j0 H j H j0
N S
þ V X
N R
r i DH R i ¼ UA H ðT c TÞ W s
(5.97)
j¼1
i¼1
Thus, the energy balance equation can be solved simultaneously with the mole balance equa-
tion to determine the reactor output or reactor volume requirement.
For a steady PFR, Eqn (3.134) is reduced to
X
N S
X
N R
d Q
d W s
F j0 dH j þ
r i DH Ri d V ¼
(5.98)
j¼1
i¼1
W s ¼
Usually, the shaft work is not present or negligible in a PFR,
0. The heat transferred into
the reactor can be written in the same manner as for a CSTR:
d Q ¼ Ua T c T d V
(5.99)
where a is the specific heat transfer area, which equals the heat transfer area divided by the
reactor volume. Thus, the energy balance equation for a steady PFR is given by
X
N S
X
N R
F j0 C Pj dT þ
r i DH R i d V ¼ UaðT c
d V
(5.100)
j¼1
i¼1
which is a differential equation, just like the mole balance equation for PFR.
Example 5-9. The exothermic gas phase reaction:
k f
k b
%
þ
r ¼ k f p A k b p B p C
A
B
C
is carried out in a CSTR operating at 50 bar. Calculate the maximum rate if the reactor oper-
ates at a 22% conversion of A with a pure A in the feed. Additional data are given below
k f ¼ 0:435 exp
E f
RT
mol s 1
$m 3
$bar 1
;
E f ¼ 20 kJ
=
mol
k b ¼ 147 exp
E b
RT
mol s 1
$m 3
$bar 2
;
E b ¼ 60 kJ
=
mol
Solution: For nonisothermal reactors, temperature plays an important role in reactor perfor-
mance. In a CSTR, the temperature is uniform in the reactor and thus is the same as the final
(output) temperature. To find the maximum reaction rate, we perform:
d r
d T ¼ p A
d k f
d k b
d T
0 ¼
d T p B p C
(E5-9.1)
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