
6.4 NONISOTHERMAL OPERATIONS
The design formulation of nonisothermal batch reactors with multiple reactions fol-
lows the procedure outlined in the previous section—we write Eq. 6.1.1 for each
independent reaction. However, since the reactor temperature may vary during
the operation, we should solve the design equations simultaneously with the
energy balance equation. Note that the energy balance equation (Eq. 6.1.17) con-
tains another variable—the temperature of the heating (or cooling) fluid, u
F
, that
may also vary during the operation (u
F
is constant only when the fluid either evap-
orates or condenses). In general, we have to write the energy balance equation for
the heating/cooling fluid to express changes in u
F
, but, in most batch reactor appli-
cations, u
F
is assumed constant. Because of the complex geometry of the heat-
transfer surface (shell or coil), the average of the inlet temperature and the outlet
temperature is usually used.
The procedure for setting up the energy balance equation goes as follows:
1. Define the reference state, and identify T
0
, C
0
,(N
tot
)
0
, and its species compo-
sitions, y
j
0
’s. Recall that, in most applications, the initial state is selected as
reference state.
2. Determine the specific molar heat capacity of the reference state,
^
c
p
0
.
3. Determine the dimensionless activation energies, g
i
’s, of all chemical
reactions.
4. Determine the dimensionless heat of reactions, DHR
m
’s, of each independent
reaction.
5. Determine the correction factor of the heat capacity, CF(Z
m
, u).
6. Determine (or specify) the dimensionless temperature of the heating/cooling
fluid, u
F
.
7. Specify the dimensionless heat-transfer number, HTN (using Eq. 6.1.26).
8. Determine (or specify) the initial dimensionless temperature, u(0).
9. Solve the energy balance equation simultaneously with the design equations
to obtain Z
m
’s and u as functions of the dimensionless operating time, t.
The design formulation of nonisothermal batch reactors consists of n
I
þ 1 non-
linear first-order differential equations whose initial values are specified. The sol-
utions of these equations provide Z
m
’s and u as functions of t. The examples
below illustrate the design of nonisothermal ideal batch reactors.
Example 6.12 The first-order, liquid-phase endothermic reactions
Reaction 1: A ! 2B
Reaction 2: B ! 2C þ D
216 IDEAL BATCH REACTOR