In the previous section, we derived Equation (11-28), which relates conversion to temperature and the heat added to the reactor, . Let’s stop a minute and consider a system with the special set of conditions of no work, , adiabatic operation , let Ti0 = T0 and then rearrange (11-28) into the form
In many instances, the ΔCP(T – TR)term in the denominator of Equation (11-29) is negligible with respect to the term, so that a plot of X vs. T will usually be linear, as shown in Figure 11-2. To remind us that the conversion in this plot was obtained from the energy balance rather than the mole balance, it is given the subscript EB (i.e., XEB) in Figure 11-2.
Figure 11-2. Adiabatic temperature–conversion relationship.
Equation (11-29) applies to a CSTR, PFR, or PBR, and also to a batch (as will be shown in Chapter 13). For and , Equation (11-29) gives us the explicit relationship between X and T needed to be used in conjunction with the mole balance to solve reaction engineering problems as discussed in Section 11.1.
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