MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
MODELING CHAR OXIDATION AS A FUNCTION OF PRESSURE ...
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nobs = 1 (KCs )<br />
2<br />
2<br />
1<br />
[KCs − ln(1+ KCs )] (1 + KCs )<br />
It can be seen that the observed reaction order in Zone II (n obs) for the Langmuir rate<br />
equation is a complex function of a non-dimensional number KC s. An important<br />
49<br />
(5.13)<br />
implication of Eq. (5.13) is that the value of n obs ranges from 0.5 to 1 (see Table 5.1), just<br />
like the range of n obs in Eq. (5.8), as shown in Figure 5.1. That is, in Zone II the observed<br />
reaction order (n obs) cannot be less than 0.5 if the reaction is sufficiently described by the<br />
Langmuir rate equation, assuming the reaction rate contributed from the external surface<br />
area of the particle is negligible compared to that from the internal surface area. Similarly,<br />
the observed reaction order can be estimated from Eqs. (5.11), (5.9) and (5.5):<br />
1 KCs 1<br />
nobs = +<br />
1+ KC 1<br />
[1−<br />
s 2KCs +<br />
2(1+ KC ) s<br />
1 + KCs 2 ] (5.14)<br />
or from Eqs. (5.12), (5.9) and (5.5):<br />
1<br />
nobs =<br />
1+ KCs + KC s<br />
2KC s +1<br />
(5.15)<br />
Table 5.1. The values of n obs at different values of KC s based on the standard<br />
general modulus and simpler general moduli<br />
KCs 0 0.125 0.25 1 4 16 64 ∞<br />
nobs from (5.13) 1.00<br />
*<br />
0.962 0.931 0.815 0.669 0.572 0.527 0.500<br />
nobs from (5.14) 1.00 0.955 0.931 0.850 0.678 0.557 0.515 0.500<br />
nobs from (5.15) 1.00 0.989 0.967 0.833 0.644 0.544 0.512 0.500<br />
* Note: Zero divided by zero situation. Value exists only in the limit.<br />
The theory developed above provides a new way to estimate the kinetic<br />
parameter K in the Langmuir rate equation. By measuring the observed reaction order in