Ideal Reactors for a Single ReactionIn nonisothermal operations energy balances must be used in conjunction with material balances.. Ideal Reactors for a Single ReactionIn this chapter w
Trang 1Chemical Reaction Engineering
(Homogeneous Reactions in Ideal Reactors)
Mai Thanh Phong, Ph.D.
VIETNAM NATIONAL UNIVERSITY – HO CHI MINH CITY UNIVERSITY OF TECHNOLOGY
FACULTY OF CHEMICAL ENGINEERING
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1 Material and energy balances
The starting point for all design is the material balance expressed for any
reactant (or product)
Thus, as illustrated in Fig 3.1, we have
Figure 3.1 Material
balance for an element
of volume of the reactor
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In nonisothermal operations energy balances must be used in conjunction with
material balances
Thus, as illustrated in Fig 3.2, we have
Figure 3.2 Energy balance for
an element of volume
of the reactor
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In this chapter we develop the performance equations for a single fluid reacting
in the three ideal reactors shown in Fig 3.3 We call these homogeneous
reactions
Figure 3.3 The three types of ideal reactors: (a) batch reactor, or BR; (b) plug
flow reactor, or PFR; and (c) continuously stirred tank reactor, or CSTR.
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2 Batch reactor (BR)
Make a material balance for any component A Noting that no fluid enters or
leaves the reaction mixture during reaction, the material balance written for
component A is
or
(3.1)
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By replacing these two terms in Eq 3.1, we obtain
(3.3) Rearranging and integrating then gives
If the density of the fluid remains constant, we obtain
n
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For all reactions in which the volume of reacting mixture changes
proportionately with conversion, Eq 3.4 becomes
3 Continuously stirred tank reactor (CSTR)
Figure 3.4 Notation for a CSTR
r Af = r A
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By selecting reactant A for consideration, material balance for a CSTR can be written as follows
As shown in Fig 3.4, if F A0 = v 0 C A0 is the molar feed rate of component A to
the reactor, then considering the reactor as a whole we have
(3.7)
Introducing these three terms into Eq 3.7, we obtain
(3.8)
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which on rearrangement becomes
(3.9)
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More generally, if the feed on which conversion is based, subscript 0, enters
the reactor partially converted, subscript i, and leaves at conditions given by
subscript f, we have
(3.10)
For the case of constant-density systems X A = 1 – CA/CA0:
(3.11)
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Figure 3.5 is a graphical representation of these mixed flow performance
equations
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4 Plug flow tubular reactor (PFTR)
At the steady-state, the material balance for reactant A becomes
Figure 3.6 Notation for a plug
flow tubular reactor
(3.12)
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Referring to Fig 3.6, we see for volume dV that
Introducing these three terms into Eq 3.12, we obtain
Noting that
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For the reactor as a whole the expression must be integrated Grouping the terms accordingly, we obtain
Thus
(3.14)
For a more general expression, we have
(3.15)
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For the special case of constant-density systems
We have
(3.16)
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Figure 3.7 Graphical representation of the performance equations for plug flow
tubular reactors
Fig 3.7 displays these performance equations and shows that the space-time
needed for any particular duty can always be found by numerical or graphical
3.14
3.16