Consider two parallel first-order reactions:
As we have seen in Chapter 1, for a batch reactor the selectivity is defined by:
but
Hence the selectivity without diffusion limitation can be written:
(without diffusion limitation)
The denominator does not need to be clarified. Its value depends on what is considered as an ideal case. This could be, for example:
If intraparticulate diffusion becomes extensive, since each of the reactions can develop independently of the other, we have to take account of two independent efficiency factors h1 and h2 so that:
(with diffusion limitation) =
and
If these diffusion limitations are severe, both for and for , the will be inversely proportional to , and we can write:
(10.30)
can be higher than depending on the respective values of , and .
10.5.2. Twin first-order reactions
Consider the system of twin reactions represented by:
For a batch reactor, the instantaneous selectivity is written by definition
because represents the maximum number of moles of A2 which could be obtained per mole of A1 if reaction 2 did not occur:
If intraparticulate diffusion intervenes significantly to limit the penetration rate of a), we can define a Thiele modulus:
and an efficiency
so that
(10.31)
As foreseeable, the diffusion limitation has no effect on the selectivity of twin reactions.
10.5.3. Consecutive reactions
Consider the reactions:
By definition, the instantaneous selectivity for a batch reactor is:
because represents the maximum number of moles of A2 which could be obtained per mole of A1 if reaction 2 did not occur.
Selectivity without diffusion limitation is written:
Hence if we define
(10.32)
The integrated selectivity:
is obtained by integrating (10.32). To do this, we can write:
The result of this integration, using the assumption w^o = 0> i-s- "o intermediate compound in the reactor feed, leads to:
or
and since
In these conditions:
(10.33)
and
If the reactions are both clearly affected by intraparticulate diffusion, we can show that the instantaneous selectivity is written [2]:
(10.34)
where
= molar flux of A2 leaving the grain,
= molar flux of A1 entering the grain,
= ratio of the two fluxes in an ideal situation.
Knowing also that:
we can calculate the integrated selectivity
by writing
Integrating, and using the assumption , this gives:
and consequently
(10.35)
and
If m is larger than 1, which frequently occurs, selectivity with diffusion limitation is lower. For values of m of around 10, a 50 per cent loss of selectivity can be observed. Decreasing the particle size helps to offset this loss of selectivity, at least partially.
Note a particular feature of expression (10.34). At the very start of the reaction, we normally expect to observe only the appearance of A2, without the occurrence of the subsequent reaction, and consequently an initial selectivity of 1.
In the case of a pronounced diffusion limitation, it is observed that the initial selectivity is equal to , which means that, from the outset of the reaction, product A3 appears resulting from the disappearance of A2. This clearly indicates that A2, trapped in the pores, cannot escape from them without damage and is subject to the subsequent reaction, so that even the first observation concerning the interior of the fluid phase reveals the product resulting from the disappearance of A2. This process can be exploited to identify a possible diffusion limitation.
[1] The notation N1 refers to the molar flux of A1 per unit of interfacial area. The notation N1 refers to the molar flux of A1 per grain.
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